(Mamoru Tanahashi) Department of Mechanical and Aerospaoe Engineering Tokyo Institute of Technology ,,., ,, $\sim$,,

Size: px
Start display at page:

Download "(Mamoru Tanahashi) Department of Mechanical and Aerospaoe Engineering Tokyo Institute of Technology ,,., ,, $\sim$,,"

Transcription

1 (Mamoru Tanahashi) Department of Mechanical and Aerospaoe Engineering Tokyo Institute of Technology $\sim$ ) 2) 3) (DNS) DNS DNS 8 8 $(\eta)$ 8 (ud 12 Fig 1 Distribution of coherent fine scale eddy in homogeneous isotropic turbulence for $Re_{\lambda}=2876$

2 $\frac{1}{\eta}=\frac{re_{\lambda}^{3/2}}{15^{3 4}}$ 70 Fig 2 Schematic of coherent fine scale eddy in homogeneous turbulence 2 4) 5) 6) 7) 3) 2 DNS $\nabla\cdot u=0$ $\frac{\partial u}{\partial l}+(u\cdot\nabla)u=-\nabla p+\frac{1}{re}\nabla^{2}u$ $u$ $p$ $Re$ ( Re$\lambda$ $Re_{\lambda}>100$ $N^{3} \propto(\frac{re_{\lambda}^{3/2}}{15^{3 4}}1^{3}$

3 channel $\ll_{s}^{*}\approx^{\approx}$ : 71 1 DNS HIT: TML: SML: TCF: Channel $Re_{\lambda}$ TTC:Taylor-Couette : $Re_{\iota 00}$ : $Re_{\tau}$ : $\Lambda$ Rei : $\delta$ Fig 3 Joint probability density function of diameter and maximum azimuthal velocity of coherent fine scale eddy in homogeneous isotropic turbulence $-5/3$ DNS 680 (4096X4096X4096) DNS8) DNS9)10) TS$UBmB$ 1 TSUBEME DNS $-5/3$ 1 DNS

4 72 Flg 4 coherent $n_{1\sigma t^{r}\cdot but\cdot O^{\eta}O }^{-}$ $\sigma fine ca^{1}e$ eddv $:_{n} 1y[:g\cdot g$ laycr Fig 5 Fine scale structures in turbulent channel flow Fig 6 Fine scale structures in turbulent Taylor-Couette flow 3 DNS 11) $\sim$ 20 ( 3 4 ) $\sim$ ( ) 6 7 ( $\tilde\sim$ ) ( ) $\sim$ ) 4 DNS 12) DNS

5 73 DNS 1 4 DNS 3) 9) 5 DNS 1 4 ( ) ) $s$ ( $)$ 3) 6 DNS 13) DNS $13\rangle$ 3 11) 14) 15) 7

6 $\ddagger n$ a $\geq a_{\sim}^{e}$ $\tilde{\approx}\geq^{6}$ 74 (a) (b) oo $S0$ 100 $E]<E_{t}>$ $E_{\tau}$ Fig 9 Joint probability density functions of energy transfer and number density ofthe diameter above $80\eta$ cube of integral length scale unit (a) and (b) are conditioned by local Kolmogorov scale $\eta_{i}$ Fig 1 $\Delta$ eddies (a) and contour surfaces of high strain rate in large scale for filter size $\eta$ and 320 (yellow) with the axes (b) scale are $80\eta$ (red) $160\eta$ (orange) 8 80 $\eta$ 7 8 ${\rm Re}_{\lambda}=2227(a)$ 2561 (b) 2876(c) $\pi$ XTEzXy-c/12(yc $\sim$ -31B) $Q_{c}$ 8 $Q_{c}$ GS SGS E$\tau$ 80 $\eta$ $E_{\tau}=-\tau_{j/}\overline{S}_{ij}=-L_{ijj^{-C_{i/}\overline{S}_{1j}-R_{ljj}}}F_{j}S_{j}$ $L_{j}i$ $C_{jj}$ $R_{ij}$ $320\eta(\approx 088i_{E})$ $N$ ( $\eta$1)11) 9(a) $\eta_{f}/\eta>1o$ 9(b) $\eta_{1}/\eta<10$ $\eta_{l}/\eta>10$ $\eta_{i}/\eta<10$ GS-SGS

7 75 80 $\eta$ GS-SGS ) $ /$ 10(a) 7(b) GS-SGS GS SGS 10(a) GS-SGS $E$ Forward scatter 80 $\eta$ GS-SGS 10(b) $80\eta$ 160 $\eta$ 320 $\eta$ 15) Large Eddy Simulation SGS 15) 4 16) 11 $331l_{E^{x}}3311_{E^{X}}331I_{E}(Re_{\lambda}=2227)$ $317i_{E^{x}}317l_{E}\cross 3171_{E}$ $({\rm Re}_{\lambda}=2561)$ $Q=(W_{ij}W_{rj}\cdot- S_{ij}S_{1_{j}})/2$ ) $s$ PDF variance $17$ ) $ 8)$ PDF variance (PDF) PDF PDF variance $D( a\eta\cdot Q)=\sum_{n\cdot 0}^{Ne}(P_{\alpha\eta}(n\cdot Q)-P_{1ln\prime to;m}(n\cdot Q)f$

8 $\bigotimes_{\hslash\s}\triangleright$ $\otimes\zeta\ddot{\triangleright}r$ 76 (a) (b) Fig 12 Cell-scale and eddy-intensity dependences of PDF variance of the coherent fine scale eddy for $Re_{\lambda}=2227(a)$ and 2561 (b) a $\eta$ $P_{8t}/n:Q)$ $Q_{c}$ $Q_{c}>Q$ PDF $P_{unir\circ rm}(n:q)$ PDF PDF variance 12 $Q_{c}$ PDF variance 19) 1/ - $Q_{c}$ PDF variance $Re_{\lambda}=2227$ $\partial \mathcal{t}^{-}14\eta$ $Re_{\lambda}=2561$ at16 $\eta$ $\lambda=293\eta$ $31$ 6 $\eta$ PDF variance 1/2 $Q_{c}$ $Q_{c}$ 12 $Q_{c}$ PDF variance

9 77 PDF variance 11 $Q_{c}$ PDF variance PDF variance $Re_{\lambda}=2227$ $Q_{c}/(u_{rm}J\eta)^{2}>017$ $Re_{\lambda}=2561$ $Q_{c}/(u_{rms}/\eta)\underline$ $>025$ $\partial tf^{128\eta}$ $143$ $\eta$ $Re_{\lambda}=2227$ 2561 DNS PDF variance 11 (a) ) 15 $-1$ DNS ) 8 21)

10 78 $22$ ) $23)$ 24) 25) 6 $)$ 1 M Tanahashi T Miyauchi and J Ikeda: Identification of Coherent Fine Scale Structure in Turbulence IUTAM Symp: Simulation and Identification of Organized Structures in Flows pp $)$ M Tanahashi S Iwase and T Miyauchi: Appearance and Alignment with Strain Rate of Coherent Fine Scale Eddies in Turbulent Mixing Layer J Turbulence 2 No $)$ 3 M Tanahashi S -J Kang T Miyamoto S Shiokawa and T Miyauchi: Scaling Law of Fine Scale Eddies in Turbulent Channel Flows up to Int J Heat and Fluid Flow $Rc_{\iota}=800$ 25 pp $)$ 4 : (B ) 68 pp $)$ 5 : Thermal Science and Engineering 8 pp $)$ M Sato M Tanahashi and T Miyauchi: Droplet Dispersion and Vapor Mixing by Fine Scale Turbulence $I$nt J Heat and Fluid Flow to be submitted $)$ M Tanahashi M Fujimura and T Miyauchi: Coherent Fine Scale Eddies in Turbulent Premixed Flames Proc Combust Inst 28 pp $)$ Y Kaneda T lshihara M Yokokawa K Itakura and A Uno: Energy Dissipation Rate and Energy Spectrum in High Resolution Direct NumericaI Simulations of Turbulence in a Periodic Box Phys Fluids 15 ppl21-l $)$ 9 : 2005 AM ) T Tsukahara H Kawamura and K Shingai: DNS of Turbulent Couette Flow with Emphasis on the Large $\cdot$scale Structure in the Core Region J Turbulence 7 No ) : 18 (CD-ROM) A ) Y Wang M Tanahashi and T Miyauchi: Coherent Fine Scale Eddies in Turbulence Transition of Spatially-Developing Mixing Layer Int J Heat and Fluid Flow to be submitted ) Taylor-Couette 20 (CD-ROM) A ) : 19

11 79 (CD-ROM) E ) M Tanahashi K Fujibayashi and T Miyauchi Fine Scale Eddy Cluster and Energy Cascade in Homogeneous Isotropic Turbulence IUTAM Bookseries (IUTAM Symposium on Computational Physics and New Perspectives in Turbulence) Vol 4 pp ) : 21 (CD-ROM) E ) L-P Wang M R Maxey: Settling Velocity and Concentration Distribution of Heavy Particles In Homogeneous Isotropic Turbulence J Fluid Mech 256 pp ) R C Hogan J N Cuzzi: Stokes and Reynolds Number Dependence of Preferential Particle Concentration in Simulated Three-Dimensional Turbulence Physics of Fluids pp 293S ) : Thermal Science and Engineering 8-3 pp ) T Michioka and S Komori: Large-Eddy Simulation of a Turbulent Reacting Liquid Flow AlChE Joumal 50 pp $2705\cdot 2720$ ) M Tanahashi Y Wang T Fujisawa K Chinda and T Miyauchi: Fractal Geometry and Mixing Transition in Turbulent Mixing Layer Proc 5th Int Symp on Turbulence and Shear Flow Phenomena ) T Kajishima: Influence of Particle Rotation on the Interaction between Particle Clusters and Particle-lnduced Turbulence Int J Heat and Fluid Flow 25 pp ) B Yu and Y Kawaguchi: DNS of Fully Developed Turbulent Heat Transfer of a Viscoelastic Drag-Reducing Flow lnt J Heat and Mass Transfer 48 pp ) M Tanahashi Y Nada Y lto and T Miyauchi: Local Flame Structure in the Well-Stirred Reactor Regime Proc Combust Inst 29 pp ) : 25 pp

$\hat{\grave{\grave{\lambda}}}$ $\grave{\neg}\backslash \backslash ^{}4$ $\approx \mathrm{t}\triangleleft\wedge$ $10^{4}$ $10^{\backslash }$ $4^{\math

$\hat{\grave{\grave{\lambda}}}$ $\grave{\neg}\backslash \backslash ^{}4$ $\approx \mathrm{t}\triangleleft\wedge$ $10^{4}$ $10^{\backslash }$ $4^{\math $\mathrm{r}\mathrm{m}\mathrm{s}$ 1226 2001 76-85 76 1 (Mamoru Tanahashi) (Shiki Iwase) (Toru Ymagawa) (Toshio Miyauchi) Department of Mechanical and Aerospaoe Engineering Tokyo Institute of Technology

More information

チャネル乱流における流体線の伸長

チャネル乱流における流体線の伸長 69 d(l/l )/dt y + = 15 Re τ = 18 395 Kolmogorov τ η.1.18 Kolmogorov.65τ η,min 1 Stretching Rate of Material Lines in Turbulent Channel Flow Takahiro TSUKAHARA, Faculty of Science and Technology, Tokyo

More information

20 $P_{S}=v_{0}\tau_{0}/r_{0}$ (3) $v_{0}$ $r_{0}$ $l(r)$ $l(r)=p_{s}r$ $[3 $ $1+P_{s}$ $P_{s}\ll 1$ $P_{s}\gg 1$ ( ) $P_{s}$ ( ) 2 (2) (2) $t=0$ $P(t

20 $P_{S}=v_{0}\tau_{0}/r_{0}$ (3) $v_{0}$ $r_{0}$ $l(r)$ $l(r)=p_{s}r$ $[3 $ $1+P_{s}$ $P_{s}\ll 1$ $P_{s}\gg 1$ ( ) $P_{s}$ ( ) 2 (2) (2) $t=0$ $P(t 1601 2008 19-27 19 (Kentaro Kanatani) (Takeshi Ogasawara) (Sadayoshi Toh) Graduate School of Science, Kyoto University 1 ( ) $2 $ [1, ( ) 2 2 [3, 4] 1 $dt$ $dp$ $dp= \frac{dt}{\tau(r)}=(\frac{r_{0}}{r})^{\beta}\frac{dt}{\tau_{0}}$

More information

NUMERICAL CALCULATION OF TURBULENT OPEN-CHANNEL FLOWS BY USING A MODIFIED /g-e TURBULENCE MODEL By Iehisa NEZU and Hiroji NAKAGA WA Numerical calculat

NUMERICAL CALCULATION OF TURBULENT OPEN-CHANNEL FLOWS BY USING A MODIFIED /g-e TURBULENCE MODEL By Iehisa NEZU and Hiroji NAKAGA WA Numerical calculat NUMERICAL CALCULATION OF TURBULENT OPEN-CHANNEL FLOWS BY USING A MODIFIED /g-e TURBULENCE MODEL By Iehisa NEZU and Hiroji NAKAGA WA Numerical calculation techniques of turbulent shear flows are classified

More information

Fig. 1 Experimental apparatus.

Fig. 1 Experimental apparatus. Effects of Concentration of Surfactant Solutions on Drag-Reducing Turbulent Boundary Layer In this study, the influence of a drag-reducing surfactant on the turbulent boundary layer was extensively investigated

More information

60 1: (a) Navier-Stokes (21) kl) Fourier 2 $\tilde{u}(k_{1})$ $\tilde{u}(k_{4})$ $\tilde{u}(-k_{1}-k_{4})$ 2 (b) (a) 2 $C_{ijk}$ 2 $\tilde{u}(k_{1})$

60 1: (a) Navier-Stokes (21) kl) Fourier 2 $\tilde{u}(k_{1})$ $\tilde{u}(k_{4})$ $\tilde{u}(-k_{1}-k_{4})$ 2 (b) (a) 2 $C_{ijk}$ 2 $\tilde{u}(k_{1})$ 1051 1998 59-69 59 Reynolds (SUSUMU GOTO) (SHIGEO KIDA) Navier-Stokes $\langle$ Reynolds 2 1 (direct-interaction approximation DIA) Kraichnan [1] (\S 31 ) Navier-Stokes Navier-Stokes [2] 2 Navier-Stokes

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

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

Microsoft Word - 中間報告書12-NA10.doc

Microsoft Word - 中間報告書12-NA10.doc 12-NA10,,,,. (DNS) (1) DNS (2)n 3 DNS (3) 4 1 2 学際大規模情報基盤共同利用 共同研究拠点 平成 24 年度共同研究 中間報告書 2012 年 12 月 後藤俊幸 名古屋工業大学創成シミュレーション Box 乱流 地球シミュレータを用いて実施した 工学専攻 一様等方性乱流の高効率な世界最大規模 DNS(格子 大規模 DNS コード開発 DNS の実施 点数

More information

液相化学反応を伴う乱流拡散の研究名城大学理工学部研究報告 No.5 21 R 6 R S 1) B 6 2 M =1 Nozzle ID =1.2 OD = x mm 6 mm 6 mm 2 mm M = 1 mm mm 1.5 mm x 1 x = 1 m

液相化学反応を伴う乱流拡散の研究名城大学理工学部研究報告 No.5 21 R 6 R S 1) B 6 2 M =1 Nozzle ID =1.2 OD = x mm 6 mm 6 mm 2 mm M = 1 mm mm 1.5 mm x 1 x = 1 m 1) A Study on Turbulent Diffusion with Chemical Reaction in Liquid Takashi KUBO 1) Abstract Turbulent diffusion with chemical reactions is of practical importance in many engineering and environmental

More information

溝乱流における外層の乱れの巨視的構造に関するモデル Titleシミュレーション ( 乱れの発生, 維持機構および統計法則の数理 ) Author(s) 奥田, 貢 ; 辻本, 公一 ; 三宅, 裕 Citation 数理解析研究所講究録 (2002), 1285: Issue Date

溝乱流における外層の乱れの巨視的構造に関するモデル Titleシミュレーション ( 乱れの発生, 維持機構および統計法則の数理 ) Author(s) 奥田, 貢 ; 辻本, 公一 ; 三宅, 裕 Citation 数理解析研究所講究録 (2002), 1285: Issue Date 溝乱流における外層の乱れの巨視的構造に関するモデル Titleシミュレーション ( 乱れの発生, 維持機構および統計法則の数理 ) Author(s) 奥田, 貢 ; 辻本, 公一 ; 三宅, 裕 Citation 数理解析研究所講究録 (2002), 1285: 92-99 Issue Date 2002-09 URL http://hdl.handle.net/2433/42433 Right

More information

Study of the "Vortex of Naruto" through multilevel remote sensing. Abstract Hydrodynamic characteristics of the "Vortex of Naruto" were investigated b

Study of the Vortex of Naruto through multilevel remote sensing. Abstract Hydrodynamic characteristics of the Vortex of Naruto were investigated b Study of the "Vortex of Naruto" through multilevel remote sensing. Abstract Hydrodynamic characteristics of the "Vortex of Naruto" were investigated based on the remotely sensed data. Small scale vortices

More information

カルマン渦列の発生の物理と数理 (オイラー方程式の数理 : カルマン渦列と非定常渦運動100年)

カルマン渦列の発生の物理と数理 (オイラー方程式の数理 : カルマン渦列と非定常渦運動100年) 1776 2012 28-42 28 (Yukio Takemoto) (Syunsuke Ohashi) (Hiroshi Akamine) (Jiro Mizushima) Department of Mechanical Engineering, Doshisha University 1 (Theodore von Ka rma n, l881-1963) 1911 100 [1]. 3 (B\

More information

Effect of Radiation on a Spray Jet Flame Ryoichi KUROSE and Satoru KOMORI Engineering Research Laboratory, Central Research Institute of Electric Powe

Effect of Radiation on a Spray Jet Flame Ryoichi KUROSE and Satoru KOMORI Engineering Research Laboratory, Central Research Institute of Electric Powe Effect of Radiation on a Spray Jet Flame Ryoichi KUROSE and Satoru KOMORI Engineering Research Laboratory, Central Research Institute of Electric Power Industry (CRIEPI), 2-6 - 1 Nagasaka, Yokosuka-shi,

More information

Natural Convection Heat Transfer in a Horizontal Porous Enclosure with High Porosity Yasuaki SHIINA*4, Kota ISHIKAWA and Makoto HISHIDA Nuclear Applie

Natural Convection Heat Transfer in a Horizontal Porous Enclosure with High Porosity Yasuaki SHIINA*4, Kota ISHIKAWA and Makoto HISHIDA Nuclear Applie Natural Convection Heat Transfer in a Horizontal Porous Enclosure with High Porosity Yasuaki SHIINA*4, Kota ISHIKAWA and Makoto HISHIDA Nuclear Applied Heat Technology Division, Japan Atomic Energy Agency,

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

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

128 Howarth (3) (4) 2 ( ) 3 Goldstein (5) 2 $(\theta=79\infty^{\mathrm{o}})$ : $cp_{n}=0$ : $\Omega_{m}^{2}=1$ $(_{\theta=80}62^{\mathrm{o}})$

128 Howarth (3) (4) 2 ( ) 3 Goldstein (5) 2 $(\theta=79\infty^{\mathrm{o}})$ : $cp_{n}=0$ : $\Omega_{m}^{2}=1$ $(_{\theta=80}62^{\mathrm{o}})$ 1075 1999 127-142 127 (Shintaro Yamashita) 7 (Takashi Watanabe) $\mathrm{n}\mathrm{a}\mathrm{k}\mathrm{a}\mathrm{m}\mathrm{u}\mathrm{f}\mathrm{a}\rangle$ (Ikuo 1 1 $90^{\mathrm{o}}$ ( 1 ) ( / \rangle (

More information

teionkogaku43_527

teionkogaku43_527 特集 : 振動流によるエネルギー変換 熱輸送現象と応用技術 * Oscillatory Flow in a Thermoacoustic Sound-wave Generator - Flow around the Resonance Tube Outlet - Masayasu HATAZAWA * Synopsis: This research describes the oscillatory

More information

<30345F90BC96EC90E690B65F E706466>

<30345F90BC96EC90E690B65F E706466> 15 特集 国際宇宙ステーション日本実験棟 きぼう における流体実験 * Space Experiment on the Instability of Marangoni Convection in Liquid Bridge Koichi NISHINO, Department of Mechanical Engineering, Yokohama National University 1 thermocapillary

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

s: Stokes 0: total quantity 1,2: quantity evaluated at the same velocity Literature 1) Bird, R. B., et al.: "Transport Phenomena", p.62(1960),j ohn Wi

s: Stokes 0: total quantity 1,2: quantity evaluated at the same velocity Literature 1) Bird, R. B., et al.: Transport Phenomena, p.62(1960),j ohn Wi s: Stokes 0: total quantity 1,2: quantity evaluated at the same velocity Literature 1) Bird, R. B., et al.: "Transport Phenomena", p.62(1960),j ohn Wiley & Sons, Inc. 2) Chujo, K.: Dainippon Yogyokyokwai

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

カルマン渦列の消滅と再生成のメカニズム

カルマン渦列の消滅と再生成のメカニズム 1822 2013 97-108 97 (Jiro Mizushima) (Hiroshi Akamine) Department of Mechanical Engineering, Doshisha University 1. [1,2]. Taneda[3] Taneda 100 ( d) $50d\sim 100d$ $100d$ Taneda Durgin and Karlsson[4]

More information

プラズマ核融合学会誌11月【81‐11】/小特集5

プラズマ核融合学会誌11月【81‐11】/小特集5 Japan Atomic Energy Agency, Ibaraki 311-0193, Japan 1) Kyoto University, Uji 611-0011, Japan 2) National Institute of Advanced Industrial Science and Technology, Tsukuba 305-8569, Japan 3) Central Research

More information

IEEE HDD RAID MPI MPU/CPU GPGPU GPU cm I m cm /g I I n/ cm 2 s X n/ cm s cm g/cm

IEEE HDD RAID MPI MPU/CPU GPGPU GPU cm I m cm /g I I n/ cm 2 s X n/ cm s cm g/cm Neutron Visual Sensing Techniques Making Good Use of Computer Science J-PARC CT CT-PET TB IEEE HDD RAID MPI MPU/CPU GPGPU GPU cm I m cm /g I I n/ cm 2 s X n/ cm s cm g/cm cm cm barn cm thn/ cm s n/ cm

More information

133 1.,,, [1] [2],,,,, $[3],[4]$,,,,,,,,, [5] [6],,,,,, [7], interface,,,, Navier-Stokes, $Petr\dot{o}$v-Galerkin [8], $(,)$ $()$,,

133 1.,,, [1] [2],,,,, $[3],[4]$,,,,,,,,, [5] [6],,,,,, [7], interface,,,, Navier-Stokes, $Petr\dot{o}$v-Galerkin [8], $(,)$ $()$,, 836 1993 132-146 132 Navier-Stokes Numerical Simulations for the Navier-Stokes Equations in Incompressible Viscous Fluid Flows (Nobuyoshi Tosaka) (Kazuhiko Kakuda) SUMMARY A coupling approach of the boundary

More information

IPSJ SIG Technical Report Vol.2014-ARC-213 No.24 Vol.2014-HPC-147 No /12/10 GPU 1,a) 1,b) 1,c) 1,d) GPU GPU Structure Of Array Array Of

IPSJ SIG Technical Report Vol.2014-ARC-213 No.24 Vol.2014-HPC-147 No /12/10 GPU 1,a) 1,b) 1,c) 1,d) GPU GPU Structure Of Array Array Of GPU 1,a) 1,b) 1,c) 1,d) GPU 1 GPU Structure Of Array Array Of Structure 1. MPS(Moving Particle Semi-Implicit) [1] SPH(Smoothed Particle Hydrodynamics) [] DEM(Distinct Element Method)[] [] 1 Tokyo Institute

More information

42 1 Fig. 2. Li 2 B 4 O 7 crystals with 3inches and 4inches in diameter. Fig. 4. Transmission curve of Li 2 B 4 O 7 crystal. Fig. 5. Refractive index

42 1 Fig. 2. Li 2 B 4 O 7 crystals with 3inches and 4inches in diameter. Fig. 4. Transmission curve of Li 2 B 4 O 7 crystal. Fig. 5. Refractive index MEMOIRS OF SHONAN INSTITUTE OF TECHNOLOGY Vol. 42, No. 1, 2008 Li 2 B 4 O 7 (LBO) *, ** * ** ** Optical Scatterer and Crystal Growth Technology of LBO Single Crystal For Development with Optical Application

More information

Vol.7 No.2 ( ) in mm m/s 40 m/s 20 m/s m/s 20m/s 1999 US ,

Vol.7 No.2 ( ) in mm m/s 40 m/s 20 m/s m/s 20m/s 1999 US , Vol.7 No.2 (136-151) KAWAZOE Yoshihiko 13 1991; 1993; 1994; 2001; 2002e; 2003-136 - Vol.7 No.2 (136-151) 27 27 137 in 2 32 812mm 1997 2000 29 2030 m/s 40 m/s 20 m/s 0.48 14 25 m/s 20m/s 1999 US 2000 2001

More information

$arrow$ $\yen$ T (Yasutala Nagano) $arrow$ $\yen$ ?,,?,., (1),, (, ).,, $\langle$2),, (3),.., (4),,,., CFD ( ),,., CFD,.,,,

$arrow$ $\yen$ T (Yasutala Nagano) $arrow$ $\yen$ ?,,?,., (1),, (, ).,, $\langle$2),, (3),.., (4),,,., CFD ( ),,., CFD,.,,, 892 1995 105-116 105 $arrow$ $\yen$ T (Yasutala Nagano) $arrow$ $\yen$ - 1 7?,,?,, (1),, (, ),, $\langle$2),, (3),, (4),,,, CFD ( ),,, CFD,,,,,,,,, (3), $\overline{uv}$ 106 (a) (b) $=$ 1 - (5), 2,,,,,

More information

<4D F736F F D208F4390B38DC58F49938A8D6595A CA90858D48985F95B F8F43959C82B382EA82BD B5F2E646F6378>

<4D F736F F D208F4390B38DC58F49938A8D6595A CA90858D48985F95B F8F43959C82B382EA82BD B5F2E646F6378> ,54,20102 CHARACTERISTICS OF COHERENT STRUCTURE IN COMPOUND OPEN CHANNEL FLOWS WITH DEEP FLOOD PLAIN DEPTH 1 2 3 Katsutoshi WATANABE, Yousuke TOKUMITSU, Haruka YOSHINAGA 1 745-8585 3538 2 3 733-0812 13-7-502

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

第6章_田辺.PDF

第6章_田辺.PDF ( ) ( ) ( ) Tube . MGLAB 1.5 mm ( ) NS u u x u u u u = u + u ( ) ( u + u ) u u u u = u + u x x x + NS u ( ρ s ρ ) g a F R = αv 0 FR V a a a k0 k /0 MGLAB - ( ) NS CPU khz 1 10 5 NS 1 ga ARFAcoustic Radiation

More information

A Higher Weissenberg Number Analysis of Die-swell Flow of Viscoelastic Fluids Using a Decoupled Finite Element Method Iwata, Shuichi * 1/Aragaki, Tsut

A Higher Weissenberg Number Analysis of Die-swell Flow of Viscoelastic Fluids Using a Decoupled Finite Element Method Iwata, Shuichi * 1/Aragaki, Tsut A Higher Weissenberg Number Analysis of Die-swell Flow of Viscoelastic Fluids Using a Decoupled Finite Element Method Iwata, Shuichi * 1/Aragaki, Tsutomu * 1/Mori, Hideki * 1 Ishikawa, Satoshi * 1/Shin,

More information

カルマン渦列の消滅と再生成 (乱流研究 次の10年 : 乱流の動的構造の理解へ向けて)

カルマン渦列の消滅と再生成 (乱流研究 次の10年 : 乱流の動的構造の理解へ向けて) 1771 2011 34-42 34 Annihilation and reincamation of Karan s vortex street (Hiroshi Al anine) (Jiro Mizushima) (Shunsuke Ohashi) (Kakeru Sugita) 1 1 1 2 2 $h$ 100 B\ enard[1] $a$ $a/h>0.366$ Kirm$4n[2]$

More information

MD $\text{ }$ (Satoshi Yukawa)* (Nobuyasu Ito) Department of Applied Physics, School of Engineering, The University of Tokyo Lennar

MD $\text{ }$ (Satoshi Yukawa)* (Nobuyasu Ito) Department of Applied Physics, School of Engineering, The University of Tokyo Lennar 1413 2005 36-44 36 MD $\text{ }$ (Satoshi Yukawa)* (Nobuyasu Ito) Department of Applied Physics, School of Engineering, The University of Tokyo Lennard-Jones [2] % 1 ( ) *yukawa@ap.t.u-tokyo.ac.jp ( )

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

$\Downarrow$ $\Downarrow$ Cahn-Hilliard (Daisuke Furihata) (Tomohiko Onda) 1 (Masatake Mori) Cahn-Hilliard Cahn-Hilliard ( ) $[1]^{1

$\Downarrow$ $\Downarrow$ Cahn-Hilliard (Daisuke Furihata) (Tomohiko Onda) 1 (Masatake Mori) Cahn-Hilliard Cahn-Hilliard ( ) $[1]^{1 $\Downarrow$ $\Downarrow$ 812 1992 67-93 67 Cahn-Hilliard (Daisuke Furihata (Tomohiko Onda 1 (Masatake Mori Cahn-Hilliard Cahn-Hilliard ( $[1]^{1}$ reduce ( Cahn-Hilliard ( Cahn- Hilliard Cahn-Hilliard

More information

圧縮性LESを用いたエアリード楽器の発音機構の数値解析 (数値解析と数値計算アルゴリズムの最近の展開)

圧縮性LESを用いたエアリード楽器の発音機構の数値解析 (数値解析と数値計算アルゴリズムの最近の展開) 1719 2010 26-36 26 LES Numerical study on sounding mechanism of air-reed instruments (Kin ya Takahashi) * (Masataka Miyamoto) * (Yasunori Ito) * (Toshiya Takami), (Taizo Kobayashi), (Akira Nishida), (Mutsumi

More information

A03-2.dvi

A03-2.dvi 14 A3-2 Numerical Analyses in the Secondary Combustion Chamber of the Ducted Rocket Engine 184-8588 2-24-16 E-mail: kikumoto@starcadmechtuatacjp Kousuke KIKUMOTO Dept of Mech Systems Eng Tokyo Noko Univ

More information

Title 改良型 S 字型風車についての数値シミュレーション ( 複雑流体の数理とシミュレーション ) Author(s) 桑名, 杏奈 ; 佐藤, 祐子 ; 河村, 哲也 Citation 数理解析研究所講究録 (2007), 1539: Issue Date URL

Title 改良型 S 字型風車についての数値シミュレーション ( 複雑流体の数理とシミュレーション ) Author(s) 桑名, 杏奈 ; 佐藤, 祐子 ; 河村, 哲也 Citation 数理解析研究所講究録 (2007), 1539: Issue Date URL Title 改良型 S 字型風車についての数値シミュレーション ( 複雑流体の数理とシミュレーション ) Author(s) 桑名, 杏奈 ; 佐藤, 祐子 ; 河村, 哲也 Citation 数理解析研究所講究録 (2007), 1539 43-50 Issue Date 2007-02 URL http//hdlhandlenet/2433/59070 Right Type Departmental

More information

二次元コルモゴロフ流における局在乱流 (乱流を介在した流体現象の数理)

二次元コルモゴロフ流における局在乱流 (乱流を介在した流体現象の数理) 数理解析研究所講究録第 2007 巻 2016 年 22-27 22 二次元コルモゴロフ流における局在乱流 京都大学理学研究科物理学宇宙物理学専攻 蛭田佳樹 $\dagger$, 藤定義 Yoshiki Hiruta, Sadayoshi Toh Division of Physics and Astronomy, Graduate School of Science Kyoto University

More information

原著_十河.indd

原著_十河.indd 51 156 2009 134-141 Journal of the Combustion Society of Japan Vol.51 No.156 (2009) 134-141 ORIGINAL PAPER 逆火限界付近における層流火炎基部の局所燃焼速度に与えるバーナ温度の影響 Influence of Burner Temperature on Local Burning Velocity

More information

The Plasma Boundary of Magnetic Fusion Devices

The Plasma Boundary of Magnetic Fusion Devices ASAKURA Nobuyuki, Japan Atomic Energy Research Institute, Naka, Ibaraki 311-0193, Japan e-mail: asakuran@fusion.naka.jaeri.go.jp The Plasma Boundary of Magnetic Fusion Devices Naka Fusion Research Establishment,

More information

IHIMU Energy-Saving Principle of the IHIMU Semicircular Duct and Its Application to the Flow Field Around Full Scale Ships IHI GHG IHIMU CFD PIV IHI M

IHIMU Energy-Saving Principle of the IHIMU Semicircular Duct and Its Application to the Flow Field Around Full Scale Ships IHI GHG IHIMU CFD PIV IHI M IHIMU Energy-Saving Principle of the IHIMU Semicircular Duct and Its Application to the Flow Field Around Full Scale Ships IHI GHG IHIMU PIV IHI Marine United Inc. ( IHIMU ) has already developed several

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

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

Microsoft Excelを用いた分子軌道の描画の実習

Microsoft Excelを用いた分子軌道の描画の実習 J. Comput. Chem. Jpn.,Vol.9, No.4, pp.177 182 (2010) 2010 Society of Computer Chemistry, Japan Microsoft Excel a*, b, c a, 790-8577 2-5 b, 350-0295 1-1 c, 305-8568 1-1-1 *e-mail: nagaoka@ehimegw.dpc.ehime-u.ac.jp

More information

Fig. 2 Pressure-temperature diagram of pure substance and mixed thel consisting of n-tridecane and n-pentane Fig. 1 Schematic of present model

Fig. 2 Pressure-temperature diagram of pure substance and mixed thel consisting of n-tridecane and n-pentane Fig. 1 Schematic of present model Cavitation Induced Breakup Model for Multicomponent Fuel Spray Authors have developed a spray model for multicomponent fuel and reported the successful model which represents batch-distillation in multicomponent

More information

SEJulyMs更新V7

SEJulyMs更新V7 1 2 ( ) Quantitative Characteristics of Software Process (Is There any Myth, Mystery or Anomaly? No Silver Bullet?) Zenya Koono and Hui Chen A process creates a product. This paper reviews various samples

More information

TM

TM NALTR-1390 TR-1390 ISSN 0452-2982 UDC 533.6.013.1 533.6.013.4 533.6.69.048 NAL TECHNICAL REPORT OF NATIONAL AEROSPACE LABORATORY TR-1390 e N 1999 11 NATIONAL AEROSPACE LABORATORY ... 1 e N... 2 Orr-Sommerfeld...

More information

Web Two-phase Flow Analyses Using Interface Volume Tracking Tomoaki Kunugi Kyoto University 1) 2) 3)

Web Two-phase Flow Analyses Using Interface Volume Tracking Tomoaki Kunugi Kyoto University   1) 2) 3) Web 11 3 2003 8 Two-phase Flow Analyses Using Interface Volume Tracking Tomoaki Kunugi Kyoto University E-mail: kunugi@nucleng.kyoto-u.ac.jp 1) 2) 3) Lagrangian 4) MAC(Marker and Cell) 5) (VOF:Volume of

More information

315 * An Experimental Study on the Characteristic of Mean Flow in Supersonic Boundary Layer Transition Shoji SAKAUE, Department of Aerospace Engineeri

315 * An Experimental Study on the Characteristic of Mean Flow in Supersonic Boundary Layer Transition Shoji SAKAUE, Department of Aerospace Engineeri 35 * An Experimental Study on the Characteristic of ean Flow in Supersonic Boundary Layer Transition Shoji SAKAUE, Department of Aerospace Engineering, Osaka Prefecture University ichio NISHIOKA, Department

More information

316 on One Hundred Years of Boundary Layer Research, Proceedings of the IUTAM Symposium held at DLR-Göttingen, Germany, 2004, (eds. G. E. A. Meier and

316 on One Hundred Years of Boundary Layer Research, Proceedings of the IUTAM Symposium held at DLR-Göttingen, Germany, 2004, (eds. G. E. A. Meier and 316 on One Hundred Years of Boundary Layer Research, Proceedings of the IUTAM Symposium held at DLR-Göttingen, Germany, 2004, (eds. G. E. A. Meier and K. R. Sreenivasan), Solid Mech. Appl., 129, Springer,

More information

多孔質弾性体と流体の連成解析 (非線形現象の数理解析と実験解析)

多孔質弾性体と流体の連成解析 (非線形現象の数理解析と実験解析) 1748 2011 48-57 48 (Hiroshi Iwasaki) Faculty of Mathematics and Physics Kanazawa University quasi-static Biot 1 : ( ) (coup iniury) (contrecoup injury) 49 [9]. 2 2.1 Navier-Stokes $\rho(\frac{\partial

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

1.7 D D 2 100m 10 9 ev f(x) xf(x) = c(s)x (s 1) (x + 1) (s 4.5) (1) s age parameter x f(x) ev 10 9 ev 2

1.7 D D 2 100m 10 9 ev f(x) xf(x) = c(s)x (s 1) (x + 1) (s 4.5) (1) s age parameter x f(x) ev 10 9 ev 2 2005 1 3 5.0 10 15 7.5 10 15 ev 300 12 40 Mrk421 Mrk421 1 3.7 4 20 [1] Grassberger-Procaccia [2] Wolf [3] 11 11 11 11 300 289 11 11 1 1.7 D D 2 100m 10 9 ev f(x) xf(x) = c(s)x (s 1) (x + 1) (s 4.5) (1)

More information

Flow Drag and Heat Transfer Characteristics of Organic Brine with Drag Reduction Surfactant in a Straight Pipe (2nd Report, Influences of Another Kind

Flow Drag and Heat Transfer Characteristics of Organic Brine with Drag Reduction Surfactant in a Straight Pipe (2nd Report, Influences of Another Kind Flow Drag and Heat Transfer Characteristics of Organic Brine with Drag Reduction Surfactant in a Straight Pipe (2nd Report, Influences of Another Kind of Organic Brine) Naoto HARUKI*5, Hideo INABA, Akihiko

More information

CFDEM DEM DEM(MPI) LIGGGHTS CFD CFD 5) 5) 5) 11) 10) β D n = βd (1) D n β D 10) 10) β = 0.2 0.5 β β β = 0.2 0.5 β = 0.2 β = 0.5 35 30 25 ( ) 20 15 10 5 0 0 0.1 0.2 0.3 0.4 0.5 0.6 β (-) β β 1) Zhu, H.P.,

More information

) [9] DNS DNS Westbrook and Dryer[10] ( ) [11] DNS Markstein Markstein Markstein Markstein Markstein [12,13] Markstein Markstein Marks

) [9] DNS DNS Westbrook and Dryer[10] ( ) [11] DNS Markstein Markstein Markstein Markstein Markstein [12,13] Markstein Markstein Marks 56 177 2014 251-257 Journal of the Combustion Society of Japan Vol.56 No.177 (2014) 251-257 ORIGINAL PAPER 爆発シミュレーションに特化した水素 空気系の総括反応モデルに関する理論的検討 Theoretical Analysis of Global Reaction Model of H 2 /air

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

Numerical Simulation for Abrupt Contraction Flow of Fiber Suspensions in Polymeric Fluid Kazunori Yasuda, Taro Nishimura* and Kiyoji Nakamura Departme

Numerical Simulation for Abrupt Contraction Flow of Fiber Suspensions in Polymeric Fluid Kazunori Yasuda, Taro Nishimura* and Kiyoji Nakamura Departme Numerical Simulation for Abrupt Contraction Flow of Fiber Suspensions in Polymeric Fluid Kazunori Yasuda, Taro Nishimura* and Kiyoji Nakamura Department of Mechanical Engineering, Osaka University, Suita,

More information

Flow Around a Circular Cylinder with Tangential Blowing near a Plane Boundary (2nd Report, A Study on Unsteady Characteristics) Shimpei OKAYASU, Kotar

Flow Around a Circular Cylinder with Tangential Blowing near a Plane Boundary (2nd Report, A Study on Unsteady Characteristics) Shimpei OKAYASU, Kotar Flow Around a Circular Cylinder with Tangential Blowing near a Plane Boundary (2nd Report, A Study on Unsteady Characteristics) Shimpei OKAYASU, Kotaro SATO*4, Toshihiko SHAKOUCHI and Okitsugu FURUYA Department

More information

Sample function Re random process Flutter, Galloping, etc. ensemble (mean value) N 1 µ = lim xk( t1) N k = 1 N autocorrelation function N 1 R( t1, t1

Sample function Re random process Flutter, Galloping, etc. ensemble (mean value) N 1 µ = lim xk( t1) N k = 1 N autocorrelation function N 1 R( t1, t1 Sample function Re random process Flutter, Galloping, etc. ensemble (mean value) µ = lim xk( k = autocorrelation function R( t, t + τ) = lim ( ) ( + τ) xk t xk t k = V p o o R p o, o V S M R realization

More information

研究成果報告書

研究成果報告書 Simulation Study of Interaction between Alfvén Eigenmodes and Energetic Particles (TAE ) TAE TAE MHD ITER We studied the interaction between Alfvén eigenmodes and energetic particles in fusion plasmas

More information

Microsoft Word - mitomi_v06.doc

Microsoft Word - mitomi_v06.doc MSS mitomi@edm.bosai.go.jp matsuoka@edm.bosai.go.jp yamazaki@edm.bosai.go.jp taniguchi@manage.nitech.ac.jp 1 MSS MSS 2 2 1 m MSS CCT CCT Fig.1 CCT b02-b0 b0-b0b-b b-b1 CCT Landsat/TM MSS S/N 21x21 21x21

More information

食品工学.indb

食品工学.indb , Vol. 11, No. 1, pp. 51-58, Mar. 2010 IH The Visualization and Quantification of the Flow in the Pan During Induction Heating and Gas Heating Haruna KAWAKAMI, Zensyu TOU, Mika FUKUOKA, and Noboru SAKAI

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

1 P2 P P3P4 P5P8 P9P10 P11 P12

1 P2 P P3P4 P5P8 P9P10 P11 P12 1 P2 P14 2 3 4 5 1 P3P4 P5P8 P9P10 P11 P12 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 & 11 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 1! 3 2 3! 4 4 3 5 6 I 7 8 P7 P7I P5 9 P5! 10 4!! 11 5 03-5220-8520

More information

main.dvi

main.dvi Vol. 8 (25 8 ) LAT PIV Development of LAT PIV Visualization Technique for Particle Fluid System Hidetaka SAOMOTO, Takashi MATSUSHIMA and Yasuo YAMADA 35-8567 1-1-1 7 35-8573 1-1-1 Mechanical behavior of

More information

SEISMIC HAZARD ESTIMATION BASED ON ACTIVE FAULT DATA AND HISTORICAL EARTHQUAKE DATA By Hiroyuki KAMEDA and Toshihiko OKUMURA A method is presented for using historical earthquake data and active fault

More information

Al-Si系粉末合金の超塑性

Al-Si系粉末合金の超塑性 Superplasticity of Al-Si P/M Alloys Satoru Ishihara, Mikio Kondoh, Kazuhiko Itoh Al-17Si-4.5Cu-0.5Mg-(06)Fe-(02)Mm ( Mm : ) (i) (ii) Si(iii) Fe (iv) Mm Al-17Si-4.5Cu-0.5Mg500 10 2 s 1 520 110 1 s 1 Si

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

Journal of the Combustion Society of Japan Vol.58 No.185 (2016) ORIGINAL PAPER 火災旋風近傍の流れに関する研究 Flow Around a Fire Whirl *

Journal of the Combustion Society of Japan Vol.58 No.185 (2016) ORIGINAL PAPER 火災旋風近傍の流れに関する研究 Flow Around a Fire Whirl * 58 185 2016 167-171 Journal of the Combustion Society of Japan Vol.58 No.185 (2016) 167-171 ORIGINAL PAPER 火災旋風近傍の流れに関する研究 Flow Around a Fire Whirl * ONISHI, Hiroyuki and KUWANA, Kazunori 992-8510 4-3-16

More information

A Numerical Study on Early Stage of Flame Kernel Development in Spark Ignition Process for Methane/Air Combustible Mixtures Shinji NAKAYA*6, Kazuo HAT

A Numerical Study on Early Stage of Flame Kernel Development in Spark Ignition Process for Methane/Air Combustible Mixtures Shinji NAKAYA*6, Kazuo HAT A Numerical Study on Early Stage of Flame Kernel Development in Spark Ignition Process for Methane/Air Combustible Mixtures Shinji NAKAYA*6, Kazuo HATORI, Mitsuhiro TSUE, Michikata KONO, Daisuke SEGAWA

More information

報告書 H22-2A-09

報告書 H22-2A-09 061-0293 1757 TEL 0133-23-1211 2.0% 0.5% in vitro QOL Quality of Life 1 MCE-400 400 mpa s Duck Algin 350M M/G 0.8 70 80 C 20% 50 C 1.0% 5 C SV-10 5 C 10 ml E TV 20H model E 1 34 R24 1 ml 5 C 30 6 12 30

More information

塗装深み感の要因解析

塗装深み感の要因解析 17 Analysis of Factors for Paint Depth Feeling Takashi Wada, Mikiko Kawasumi, Taka-aki Suzuki ( ) ( ) ( ) The appearance and quality of objects are controlled by paint coatings on the surfaces of the objects.

More information

JSME-JT

JSME-JT Advance Publication by J-STAGE 日本機械学会論文集 Transactions of the JSME (in Japanese) DOI:.299/transjsme.6-23 Received date : 8 May, 26 Accepted date : 5 July, 26 J-STAGE Advance Publication date : 22 July,

More information

1.3 (heat transfer with phase change) (phase change) (evaporation) (boiling) (condensation) (melting) (solidification) 1.4 (thermal radiation) 4 2. 1

1.3 (heat transfer with phase change) (phase change) (evaporation) (boiling) (condensation) (melting) (solidification) 1.4 (thermal radiation) 4 2. 1 CAE ( 6 ) 1 1. (heat transfer) 4 1.1 (heat conduction) 1.2 (convective heat transfer) (convection) (natural convection) (free convection) (forced convection) 1 1.3 (heat transfer with phase change) (phase

More information

untitled

untitled 700 1 2 2 3 4 5 PDF 6 7 8 9 300 400m 1:2.5 1:1.8 75 3.2 10 11 12 1) 1998 Vol1 2) 1987-1992 3) 2001-2002 1-24 4) 1996 17 6-7 5) 2000 31 587-590 6) 2002 22 13 7) 2005 2005 20 46 1 2 3 4 5 6 7 8 9 10 11

More information

(a) -4furne.ce Fig. I Schematic drawing of cooling chamber Fig. 2 Priventive gas velocity at nozzle 405

(a) -4furne.ce Fig. I Schematic drawing of cooling chamber Fig. 2 Priventive gas velocity at nozzle 405 Fig. 1 Experimental Apparatus Fig. 2 Typical Ion Distribution in COG-Air Flame Fig. 3 Relation between Steel Temperature and Reduction Time (a) -4furne.ce Fig. I Schematic drawing of cooling chamber Fig.

More information

D v D F v/d F v D F η v D (3.2) (a) F=0 (b) v=const. D F v Newtonian fluid σ ė σ = ηė (2.2) ė kl σ ij = D ijkl ė kl D ijkl (2.14) ė ij (3.3) µ η visco

D v D F v/d F v D F η v D (3.2) (a) F=0 (b) v=const. D F v Newtonian fluid σ ė σ = ηė (2.2) ė kl σ ij = D ijkl ė kl D ijkl (2.14) ė ij (3.3) µ η visco post glacial rebound 3.1 Viscosity and Newtonian fluid f i = kx i σ ij e kl ideal fluid (1.9) irreversible process e ij u k strain rate tensor (3.1) v i u i / t e ij v F 23 D v D F v/d F v D F η v D (3.2)

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

4/15 No.

4/15 No. 4/15 No. 1 4/15 No. 4/15 No. 3 Particle of mass m moving in a potential V(r) V(r) m i ψ t = m ψ(r,t)+v(r)ψ(r,t) ψ(r,t) = ϕ(r)e iωt ψ(r,t) Wave function steady state m ϕ(r)+v(r)ϕ(r) = εϕ(r) Eigenvalue problem

More information

The Phase Behavior of Monooleoylglycerol-Water Systems Mivoshi Oil & Fat Co.. Ltd. Faculty of Science and Technology, Science University of Tokyo Inst

The Phase Behavior of Monooleoylglycerol-Water Systems Mivoshi Oil & Fat Co.. Ltd. Faculty of Science and Technology, Science University of Tokyo Inst The Phase Behavior of Monooleoylglycerol-Water Systems Mivoshi Oil & Fat Co.. Ltd. Faculty of Science and Technology, Science University of Tokyo Institute of Colloid and Interface Science, Science University

More information

untitled

untitled - - GRIPS 1 traceroute IP Autonomous System Level http://opte.org/ GRIPS 2 Network Science http://opte.org http://research.lumeta.com/ches/map http://www.caida.org/home http://www.imdb.com http://citeseer.ist.psu.edu

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

[15] 1970 Chiu [16, 17] [18-22] [20] Chiu [23] [24] [25] Chiu [16, 17] Chiu G 2

[15] 1970 Chiu [16, 17] [18-22] [20] Chiu [23] [24] [25] Chiu [16, 17] Chiu G 2 Spray Combustion. Droplet Group Combustion 1. ml 20 µm 2.4 [1-12] [13] [14] 1 [15] 1970 Chiu [16, 17] [18-22] [20] Chiu [23] [24] 2. 2-1. [25] Chiu [16, 17] Chiu G 2 N: TOTAL NUMBER OF DROPLETS 9 8 7 6

More information

(Hiroshi Okamoto) (Jiro Mizushima) (Hiroshi Yamaguchi) 1,.,,,,.,,.,.,,,.. $-$,,. -i.,,..,, Fearn, Mullin&Cliffe (1990),,.,,.,, $E

(Hiroshi Okamoto) (Jiro Mizushima) (Hiroshi Yamaguchi) 1,.,,,,.,,.,.,,,.. $-$,,. -i.,,..,, Fearn, Mullin&Cliffe (1990),,.,,.,, $E 949 1996 128-138 128 (Hiroshi Okamoto) (Jiro Mizushima) (Hiroshi Yamaguchi) 1 $-$ -i Fearn Mullin&Cliffe (1990) $E=3$ $Re_{C}=4045\pm 015\%$ ( $Re=U_{\max}h/2\nu$ $U_{\max}$ $h$ ) $-t$ Ghaddar Korczak&Mikic

More information

Development of Induction and Exhaust Systems for Third-Era Honda Formula One Engines Induction and exhaust systems determine the amount of air intake

Development of Induction and Exhaust Systems for Third-Era Honda Formula One Engines Induction and exhaust systems determine the amount of air intake Development of Induction and Exhaust Systems for Third-Era Honda Formula One Engines Induction and exhaust systems determine the amount of air intake supplied to the engine, and as such are critical elements

More information

KENZOU Karman) x

KENZOU Karman) x KENZO 8 8 31 8 1 3 4 5 6 Karman) 7 3 8 x 8 1 1.1.............................. 3 1............................................. 5 1.3................................... 5 1.4 /.........................

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

非線形長波モデルと流体粒子法による津波シミュレータの開発 I_ m ρ v p h g a b a 2h b r ab a b Fang W r ab h 5 Wendland 1995 q= r ab /h a d W r ab h

非線形長波モデルと流体粒子法による津波シミュレータの開発 I_ m ρ v p h g a b a 2h b r ab a b Fang W r ab h 5 Wendland 1995 q= r ab /h a d W r ab h 土木学会論文集 B2( 海岸工学 ) Vol. 70, No. 2, 2014, I_016-I_020 非線形長波モデルと流体粒子法による津波シミュレータの開発 Development of a Tsunami Simulator Integrating the Smoothed-Particle Hydrodynamics Method and the Nonlinear Shallow Water

More information

Gravothermal Catastrophe & Quasi-equilibrium Structure in N-body Systems

Gravothermal Catastrophe & Quasi-equilibrium Structure  in N-body Systems 2004/3/1 3 N 1 Antonov Problem & Quasi-equilibrium State in N-body N Systems A. Taruya (RESCEU, Univ.Tokyo) M. Sakagami (Kyoto Univ.) 2 Antonov problem N-body study of quasi-attractivity M15 T Antonov

More information

200708_LesHouches_02.ppt

200708_LesHouches_02.ppt Numerical Methods for Geodynamo Simulation Akira Kageyama Earth Simulator Center, JAMSTEC, Japan Part 2 Geodynamo Simulations in a Sphere or a Spherical Shell Outline 1. Various numerical methods used

More information

ArF, KrF,, CO 2 ) X MFE ITER IFE ns, MJ/ ns, MJ/ ms, MJ/ ELM JT60-SA, ITER, DEMO [µm] W 65kV 2.3A [ ] Simple estimation of the threshold thermal load on divertor surface with ELM For Carbon Divertor Case

More information

Fig. 3 Flow diagram of image processing. Black rectangle in the photo indicates the processing area (128 x 32 pixels).

Fig. 3 Flow diagram of image processing. Black rectangle in the photo indicates the processing area (128 x 32 pixels). Fig. 1 The scheme of glottal area as a function of time Fig. 3 Flow diagram of image processing. Black rectangle in the photo indicates the processing area (128 x 32 pixels). Fig, 4 Parametric representation

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