COGNACのコンセプト \(COarse Grained molecular dynamics program developed by NAgoya Cooperation\)
|
|
- みさえ おとじま
- 6 years ago
- Views:
Transcription
1 COGNAC (COarse-Grained molecular dynamics program by NAgoya Cooperation) ( ),
2 0 sec -3 msec -6 sec -9 nsec -12 psec -15 fsec GOURMET SUSHI PASTA COGNAC MUFFIN fm pm nm m mm m
3 United atom model (CH 2 ) Gay-Berne potential model Bead-spring model
4
5 Molecular dynamics (MD) Ensembles»NVE» NVT,NPH,NPT (loose-coupling / extended Hamiltonian methods) Langevin dynamics Molecular mechanics (MM) Steepest descent / conjugate gradient methods
6 Bonding 2-body(bond):Harmonic,Morse,FENE,Gaussian, Polynomial,Table 3-body(angle):Theta harmonic,cosine harmonic Theta polynomial,table 4-body(torsion):Cosine polynomial,table Non-bonding pair interaction Lennard-Jones,Gay-Berne,LJ-GB, Table Electrostatic Coulomb interaction(ewald,reaction field) Dipole-dipole interaction (Reaction field)
7 : Gay-Berne - Lennard-Jones hybrid potential C CH 2 H 2 C CH 2 H 2 C CH 3 ncb (4-methyl-4 -cyanobiphenyl) Ellipsoid Sphere Smectic phase(non-polar model) Nematic phase(polar model)
8 SILK (1) SILK COGNAC SILK Python GOURMET SILK
9 SILK (2) name="mol" nummol=10 self.engine.createmolecule(name) for i in range(0, 4): self.engine.addatoms(name, "UA", "UA_PE") for i in range(0, 3): self.engine.addbonds(name, i, i+1, "BOND_PE") for i in range(0, 2): self.engine.addangles(name, i, i+1, i+2, "ANGLE_PE") for i in range(0, 1): self.engine.addtorsions(name, i, i+1, i+2, i+3, "TORSION_PE") for i in range(0, 4): self.engine.addinteractionsites(name, [i], "NB_PE", "PAIR") self.engine.setsystem(name, nummol)
10 SILK (3) name="a20b40a20" nummol=50 key="linear" sequence=[("a",20),("b",40),("a",20)] atomtype={"a":"atom1", "B":"atom2"} bondtype={"a_a":"bond1", "A_B":"bond3", "B_B":"bond2"} interactionsitetype={"a":"sitetype1", "B":"siteType2"} self.engine.makebeadspringpolym(name, nummol, key, sequence, atomtype, bondtype, interactionsitetype)
11 Action SILK gift Action GOUMET SILK Selection of diblock
12
13 COGNAC Random: Amorphous like structures Helix: Helical structures at regular lattice points Crystal: Crystal structures defined by crystal data, i.e. unit lattice, symmetric operation and fractional coordinates Semi-crystalline lamella: Semi-crystalline lamella structures consisting of a crystal phase and an amorphous phase Multi phase structure: Micro/macro phase-separeted structures of block copolymer/polymer blend obtained by SUSHI
14 mol/pdb UDF WebLab ViewerLite (TM) mol GOURMET UDF
15 UDF PDB/car/XYZ GOURMET UDF WebLab ViewerLite (TM) car
16 etc. Lees-Edwards MD»
17 Clay(laponite) - Polymer(PEO) composite clay-polymer Clay
18 20nm 20nm
19
20 Density biased Monte Carlo (DBMC) Density biased potential (DBP) SUSHI Staggered reflective boundary condition (SRBC) Lamella builder
21 ABA triblock copolymer ABA triblock copolymer SUSHI Loop/Bridge
22 ABA triblock copolymer 300% Strain BCC sphere phase εσ
23 A/B εσ ε τ elongation δε δε δε δε
24 6nm elongation
25 COGNAC C++ COGNAC UserBond1, UserAngle1 #include "userbond1.h" double UserBond1::calcforce(const Vector3d& dr, Vector3d& ftmp) { double r,delr,ene,tmp; } r=dr.length(); delr=r-r0; tmp=kconst*delr; ftmp=dr*(tmp/r); ene=0.5*tmp*delr; return ene;
26 DPD Dissipative particle dynamics (DPD) dr dt i dv = vi, dt i = f i f i F C ij = ( C D R F + + ) ij Fij Fij i j aij = 0 ( 1 r ) ( < ) ij rˆ ij rij ( r 1) ij 1, F D ij D = w ( )( ) R R r ( ) ij rˆ ij vij rˆ ij, Fij = w rij ijrˆ ij
27 Action Python molecules/atoms/bonds ABA triblock copolymers A
28 COGNAC Python»»»»»»
29 GOURMET Action GOURMET Action
30 :
31 : -
32 UDF HELP
33 COGNAC UDF unit parameters reduced mass in [amu] reduced energy in [kj/mol] reduced length in [nm].
34 COGNAC: χ MUFFIN SUSHI PASTA COGNAC
35 COGNAC : MD/MM
36 COGNAC JCII
OCTAプロジェクト:物質の多階層シミュレーション
SS HPC 2003 2003/10/03 OCTA : www.stat.cse.nagoya-u.ac.jp,, 1 SS HPC 2003 2003/10/03 OCTA Open Computational Tool for Advanced material technology 8 2 SS HPC 2003 2003/10/03 Advanced Material Technology
More informationMUFFIN3
MUFFIN - MUltiFarious FIeld simulator for Non-equilibrium system - ( ) MUFFIN WG3 - - JCII, - ( ) - ( ) - ( ) - (JSR) - - MUFFIN sec -3 msec -6 sec GOURMET SUSHI MUFFIN -9 nsec PASTA -1 psec -15 fsec COGNAC
More informationスライド タイトルなし
J-OCTA/OCTA と LAMMPS の連携によるメリット http://www.j-octa.com/ 2016 年 2 月 19 日株式会社 JSOL エンジニアリングビジネス事業部 JSOL について 社員数 1300 人 計算科学分野は 150 人 20 以上のシミュレーション, CAE(Computer Aided Engineering) ソフトウェアミクロからマクロまで 幅広いソリューション
More information4/15 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卒業研究報告 題 目 Hamiltonian 指導教員 山本哲也教授 報告者 汐月康則 平成 14 年 2 月 5 日 1
卒業研究報告 題 目 Hamiltonian 指導教員 山本哲也教授 報告者 汐月康則 平成 4 年 月 5 日 .....4.....4......6.. 6.. 6....4. 8.5. 9.6....7... 3..... 3.... 3.... 3.3...4 3.4...5 3.5...5 3.5....6 3.5.... 3.5...... 3.5...... 3 3.5.3..4 3.5.4..5
More information02-量子力学の復習
4/17 No. 1 4/17 No. 2 4/17 No. 3 Particle of mass m moving in a potential V(r) V(r) m i ψ t = 2 2m 2 ψ(r,t)+v(r)ψ(r,t) ψ(r,t) Wave function ψ(r,t) = ϕ(r)e iωt steady state 2 2m 2 ϕ(r)+v(r)ϕ(r) = εϕ(r)
More information1 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 information19 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 informationA 99% MS-Free Presentation
A 99% MS-Free Presentation 2 Galactic Dynamics (Binney & Tremaine 1987, 2008) Dynamics of Galaxies (Bertin 2000) Dynamical Evolution of Globular Clusters (Spitzer 1987) The Gravitational Million-Body Problem
More information80 4 r ˆρ i (r, t) δ(r x i (t)) (4.1) x i (t) ρ i ˆρ i t = 0 i r 0 t(> 0) j r 0 + r < δ(r 0 x i (0))δ(r 0 + r x j (t)) > (4.2) r r 0 G i j (r, t) dr 0
79 4 4.1 4.1.1 x i (t) x j (t) O O r 0 + r r r 0 x i (0) r 0 x i (0) 4.1 L. van. Hove 1954 space-time correlation function V N 4.1 ρ 0 = N/V i t 80 4 r ˆρ i (r, t) δ(r x i (t)) (4.1) x i (t) ρ i ˆρ i t
More information3 3.1 R r r + R R r Rr [ ] ˆn(r) = ˆn(r + R) (3.1) R R = r ˆn(r) = ˆn(0) r 0 R = r C nn (r, r ) = C nn (r + R, r + R) = C nn (r r, 0) (3.2) ( 2.2 ) C
3 3.1 R r r + R R r Rr [ ] ˆn(r) = ˆn(r + R) (3.1) R R = r ˆn(r) = ˆn(0) r 0 R = r C nn (r, r ) = C nn (r + R, r + R) = C nn (r r, 0) (3.2) ( 2.2 ) C nn (r r ) = C nn (R(r r )) [2 ] 2 g(r, r ) ˆn(r) ˆn(r
More information2012専門分科会_new_4.pptx
d dt L L = 0 q i q i d dt L L = 0 r i i r i r r + Δr Δr δl = 0 dl dt = d dt i L L q i q i + q i i q i = q d L L i + q i i dt q i i q i = i L L q i L = 0, H = q q i L = E i q i i d dt L q q i i L = L(q
More informationuntitled
SPring-8 RFgun JASRI/SPring-8 6..7 Contents.. 3.. 5. 6. 7. 8. . 3 cavity γ E A = er 3 πε γ vb r B = v E c r c A B A ( ) F = e E + v B A A A A B dp e( v B+ E) = = m d dt dt ( γ v) dv e ( ) dt v B E v E
More information高知工科大学電子 光システム工学科
卒業研究報告 題 目 量子力学に基づいた水素分子の分子軌道法的取り扱いと Hamiltonian 近似法 指導教員 山本哲也 報告者 山中昭徳 平成 14 年 月 5 日 高知工科大学電子 光システム工学科. 3. 4.1 4. 4.3 4.5 6.6 8.7 10.8 11.9 1.10 1 3. 13 3.113 3. 13 3.3 13 3.4 14 3.5 15 3.6 15 3.7 17
More informationCMP Technical Report No. 4 Department of Computational Nanomaterials Design ISIR, Osaka University 2 2................................. 2.2......................... 2 3 3 3................................
More informationMolecule tomic rbital bridied tomic rbital Valence Shell Electron Pair Repulsion Rule Molecular rbital 2 1+ + 1+ 1+ 1+ 2 9+ + 9+ 9+ 9+ 2 1+ 1+ 1s 1s 2 9+ 9+ 2p 2p 9+ () 2 (2p ) 2 (2p ) 2 (2p ) 1 Energ
More informationD 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株式会社ローソン 第26期中間事業報告書
1 2 3 4 5 797 429 316 1,881 7,583 204 649 334 1,950 564 459 73.10 4,836 3,535 79.05 5,113 4,042 79.96 5,683 4,544 82.41 6,252 5,152 83.47 6,649 5,550 85.75 7,016 6,016 88.45 7,378 6,526 88.95 7,583 6,745
More informationIntroduction 2 / 43
Batalin-Vilkoviski ( ) 2016 2 22 at SFT16 based on arxiv:1511.04187 BV Analysis of Tachyon Fluctuation around Multi-brane Solutions in Cubic String Field Theory 1 / 43 Introduction 2 / 43 in Cubic open
More information1 1 1 1-1 1 1-9 1-3 1-1 13-17 -3 6-4 6 3 3-1 35 3-37 3-3 38 4 4-1 39 4- Fe C TEM 41 4-3 C TEM 44 4-4 Fe TEM 46 4-5 5 4-6 5 5 51 6 5 1 1-1 1991 1,1 multiwall nanotube 1993 singlewall nanotube ( 1,) sp 7.4eV
More information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 April 30, 2009 Outline 1. 2. 3. 4. 5. 6. 2 / 260 Today s Lecture: Itinerant Magnetism 60 / 260 Multiplets of Single Atom System HC HSO : L = i l i, S = i s i, J = L +
More informationiBookBob:Users:bob:Documents:CurrentData:flMŠÍ…e…L…X…g:Statistics.dvi
4 4 9............................................... 3.3......................... 4.4................. 5.5............................ 7 9..................... 9.............................3................................4..........................5.............................6...........................
More informationIPSJ 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 informationSAXS 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 informationA2, 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 informationOutline I. Introduction: II. Pr 2 Ir 2 O 7 Like-charge attraction III.
Masafumi Udagawa Dept. of Physics, Gakushuin University Mar. 8, 16 @ in Gakushuin University Reference M. U., L. D. C. Jaubert, C. Castelnovo and R. Moessner, arxiv:1603.02872 Outline I. Introduction:
More informationADM-Hamiltonian Cheeger-Gromov 3. Penrose
ADM-Hamiltonian 1. 2. Cheeger-Gromov 3. Penrose 0. ADM-Hamiltonian (M 4, h) Einstein-Hilbert M 4 R h hdx L h = R h h δl h = 0 (Ric h ) αβ 1 2 R hg αβ = 0 (Σ 3, g ij ) (M 4, h ij ) g ij, k ij Σ π ij = g(k
More informationssp2_fixed.dvi
13 12 30 2 1 3 1.1... 3 1.2... 4 1.3 Bravais... 4 1.4 Miller... 4 2 X 5 2.1 Bragg... 5 2.2... 5 2.3... 7 3 Brillouin 13 3.1... 13 3.2 Brillouin... 13 3.3 Brillouin... 14 3.4 Bloch... 16 3.5 Bloch... 17
More information.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 informationYuzo Nakamura, Kagoshima Univ., Dept Mech Engr. perfect crystal imperfect crystal point defect vacancy self-interstitial atom substitutional impurity
perfect crystal imperfect crystal point defect vacancy self-interstitial atom substitutional impurity atom interstitial impurity atom line defect dislocation planar defect surface grain boundary interface
More information1 2 2 (Dielecrics) Maxwell ( ) D H
2003.02.13 1 2 2 (Dielecrics) 4 2.1... 4 2.2... 5 2.3... 6 2.4... 6 3 Maxwell ( ) 9 3.1... 9 3.2 D H... 11 3.3... 13 4 14 4.1... 14 4.2... 14 4.3... 17 4.4... 19 5 22 6 THz 24 6.1... 24 6.2... 25 7 26
More informationSample 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 information42 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 information¼§À�ÍýÏÀ – Ê×ÎòÅŻҼ§À�¤È¥¹¥Ô¥ó¤æ¤é¤®
email: takahash@sci.u-hyogo.ac.jp Spring semester, 2012 Outline 1. 2 / 26 Introduction : (d ) : 4f 1970 ZrZn 2, MnSi, Ni 3 Al, Sc 3 In Stoner-Wohlfarth Moriya-Kawabata (1973) 3 / 26 Properties of Weak
More informationuntitled
173 1 2 3 1 PEFC DMFC 1 CMOS beyond CMOS More than Moore IV III-V 2 MRAM FeRAM RAM ReRAM 3 4 EL FED) 1 - - DDS 4 1 2 3 4 5 5 6 2005 2006 2007 2008 WG 2010 2030 2020 2004 2011 20072011 ISO/TC229IEC/TC113
More informationglobal global mass region (matter ) & (I) M3Y semi-microscopic int. Ref.: H. N., P. R. C68, ( 03) N. P. A722, 117c ( 03) Proc. of NENS03 (to be
Gogny hard core spin-isospin property @ RCNP (Mar. 22 24, 2004) Collaborator: M. Sato (Chiba U, ) ( ) global global mass region (matter ) & (I) M3Y semi-microscopic int. Ref.: H. N., P. R. C68, 014316
More information研究室ガイダンス(H28)福山研.pdf
1 2 3 4 5 4 He M. Roger et al., JLTP 112, 45 (1998) A.F. Andreev and I.M. Lifshitz, Sov. Phys. JETP 29, 1107 (1969) Born in 2004 (hcp 4 He) E. Kim and M.H.W. Chan, Nature 427, 225 (2004); Science 305,
More informationi
009 I 1 8 5 i 0 1 0.1..................................... 1 0.................................................. 1 0.3................................. 0.4........................................... 3
More information·«¤ê¤³¤ß·²¤È¥ß¥ì¥Ë¥¢¥àÌäÂê
.. 1 10-11 Nov., 2016 1 email:keiichi.r.ito@gmail.com, ito@kurims.kyoto-u.ac.jp ( ) 10-11 Nov., 2016 1 / 45 Clay Institute.1 Construction of 4D YM Field Theory (Jaffe, Witten) Jaffe, Balaban (1980).2 Solution
More information( ) ) AGD 2) 7) 1
( 9 5 6 ) ) AGD ) 7) S. ψ (r, t) ψ(r, t) (r, t) Ĥ ψ(r, t) = e iĥt/ħ ψ(r, )e iĥt/ħ ˆn(r, t) = ψ (r, t)ψ(r, t) () : ψ(r, t)ψ (r, t) ψ (r, t)ψ(r, t) = δ(r r ) () ψ(r, t)ψ(r, t) ψ(r, t)ψ(r, t) = (3) ψ (r,
More information1 1-49 11 5 7064 ...4 1.1...5 1....7 1.3...8...9.1...10.1.1 Lennad-Jones...10.1....1....13.3...14.4...15.4.1 L-J...15.4. Hamonic...16.4.3 Multiple time step...16.5...17.6...19.6.1...19.7...0.7.1...0.7.
More informationBIT -2-
2004.3.31 10 11 12-1- BIT -2- -3-256 258 932 524 585 -4- -5- A B A B AB A B A B C AB A B AB AB AB AB -6- -7- A B -8- -9- -10- mm -11- fax -12- -13- -14- -15- s58.10.1 1255 4.2 30.10-16- -17- -18- -19-6.12.10
More informationnm (T = K, p = kP a (1atm( )), 1bar = 10 5 P a = atm) 1 ( ) m / m
.1 1nm (T = 73.15K, p = 101.35kP a (1atm( )), 1bar = 10 5 P a = 0.9863atm) 1 ( ).413968 10 3 m 3 1 37. 1/3 3.34.414 10 3 m 3 6.0 10 3 = 3.7 (109 ) 3 (nm) 3 10 6 = 3.7 10 1 (nm) 3 = (3.34nm) 3 ( P = nrt,
More informationuntitled
1 2 3 4 5 130mm 32mm UV-irradiation UV-cationic cure UV-cationic cure UV-cationic cure Thermal cationic Reaction heat cure Thermal cationic Cation Reaction heat cure Cation (a) UV-curing of
More informationThe 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 informationIPSJ SIG Technical Report NetMAS NetMAS NetMAS One-dimensional Pedestrian Model for Fast Evacuation Simulator Shunsuke Soeda, 1 Tomohisa Yam
1 1 1 1 1 NetMAS NetMAS NetMAS One-dimensional Model for Fast Evacuation Simulator Shunsuke Soeda, 1 Tomohisa Yamashita, 1 Masaki Onishi, 1 Ikushi Yoda 1 and Itsuki Noda 1 We propose the one-dimentional
More informationCHARACTERISTICS OF LOVE WAVE GENERATED AROUND A DIPPING BASEMENT By Susumu NAKAMURA, Iwao SUETOMI, Shinichi AKIYAMA and Nozomu YOSHIDA Source mechanis
CHARACTERISTICS OF LOVE WAVE GENERATED AROUND A DIPPING BASEMENT By Susumu NAKAMURA, Iwao SUETOMI, Shinichi AKIYAMA and Nozomu YOSHIDA Source mechanism and characteristics of the horizontally propagating
More informationNosé Hoover 1.2 ( 1) (a) (b) 1:
1 watanabe@cc.u-tokyo.ac.jp 1 1.1 Nosé Hoover 1. ( 1) (a) (b) 1: T ( f(p x, p y, p z ) exp p x + p y + p ) z (1) mk B T p x p y p = = z = 1 m m m k BT () k B T = 1.3 0.04 0.03 0.0 0.01 0-5 -4-3 - -1 0
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
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修士論文 物性研究 電子版 Vol. 5, No. 2, (2016 年 5 月号 ) 27-2 F14A001B
27-2 F14A001B (Molecular Dynamics: MD) Verlet (Verlet Neighbor List: VNL ) (Cell Linked List: CLL ) (VNL-CLL ) VNL MD 10 VNL ( ) CLL (2 8 26 ) CLL ( ) VNL O(N 2 ) CLL O(N 2 ) O(N) VNL-CLL VNL-CLL Verlet
More informationLLG-R8.Nisus.pdf
d M d t = γ M H + α M d M d t M γ [ 1/ ( Oe sec) ] α γ γ = gµ B h g g µ B h / π γ g = γ = 1.76 10 [ 7 1/ ( Oe sec) ] α α = λ γ λ λ λ α γ α α H α = γ H ω ω H α α H K K H K / M 1 1 > 0 α 1 M > 0 γ α γ =
More informationii 3.,. 4. F. (), ,,. 8.,. 1. (75%) (25%) =7 20, =7 21 (. ). 1.,, (). 3.,. 1. ().,.,.,.,.,. () (12 )., (), 0. 2., 1., 0,.
24(2012) (1 C106) 4 11 (2 C206) 4 12 http://www.math.is.tohoku.ac.jp/~obata,.,,,.. 1. 2. 3. 4. 5. 6. 7.,,. 1., 2007 (). 2. P. G. Hoel, 1995. 3... 1... 2.,,. ii 3.,. 4. F. (),.. 5... 6.. 7.,,. 8.,. 1. (75%)
More informationchap1_MDpotentials.ppt
simplest Morse : simplest (1 Well-chosen functional form is more useful than elaborate fitting strategies!! Phys. Rev. 34, 57 (1929 ( 2 E ij = D e 1" exp("#(r ij " r e 2 r ij = r i " r j r ij =r e E ij
More information9 1. (Ti:Al 2 O 3 ) (DCM) (Cr:Al 2 O 3 ) (Cr:BeAl 2 O 4 ) Ĥ0 ψ n (r) ω n Schrödinger Ĥ 0 ψ n (r) = ω n ψ n (r), (1) ω i ψ (r, t) = [Ĥ0 + Ĥint (
9 1. (Ti:Al 2 O 3 ) (DCM) (Cr:Al 2 O 3 ) (Cr:BeAl 2 O 4 ) 2. 2.1 Ĥ ψ n (r) ω n Schrödinger Ĥ ψ n (r) = ω n ψ n (r), (1) ω i ψ (r, t) = [Ĥ + Ĥint (t)] ψ (r, t), (2) Ĥ int (t) = eˆxe cos ωt ˆdE cos ωt, (3)
More informationpositron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) MeV : thermalization m psec 100
positron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) 0.5 1.5MeV : thermalization 10 100 m psec 100psec nsec E total = 2mc 2 + E e + + E e Ee+ Ee-c mc
More information* 1 1 (i) (ii) Brückner-Hartree-Fock (iii) (HF, BCS, HFB) (iv) (TDHF,TDHFB) (RPA) (QRPA) (v) (vi) *
* 1 1 (i) (ii) Brückner-Hartree-Fock (iii) (HF, BCS, HFB) (iv) (TDHF,TDHFB) (RPA) (QRPA) (v) (vi) *1 2004 1 1 ( ) ( ) 1.1 140 MeV 1.2 ( ) ( ) 1.3 2.6 10 8 s 7.6 10 17 s? Λ 2.5 10 10 s 6 10 24 s 1.4 ( m
More information2 (March 13, 2010) N Λ a = i,j=1 x i ( d (a) i,j x j ), Λ h = N i,j=1 x i ( d (h) i,j x j ) B a B h B a = N i,j=1 ν i d (a) i,j, B h = x j N i,j=1 ν i
1. A. M. Turing [18] 60 Turing A. Gierer H. Meinhardt [1] : (GM) ) a t = D a a xx µa + ρ (c a2 h + ρ 0 (0 < x < l, t > 0) h t = D h h xx νh + c ρ a 2 (0 < x < l, t > 0) a x = h x = 0 (x = 0, l) a = a(x,
More informationV(x) m e V 0 cos x π x π V(x) = x < π, x > π V 0 (i) x = 0 (V(x) V 0 (1 x 2 /2)) n n d 2 f dξ 2ξ d f 2 dξ + 2n f = 0 H n (ξ) (ii) H
199 1 1 199 1 1. Vx) m e V cos x π x π Vx) = x < π, x > π V i) x = Vx) V 1 x /)) n n d f dξ ξ d f dξ + n f = H n ξ) ii) H n ξ) = 1) n expξ ) dn dξ n exp ξ )) H n ξ)h m ξ) exp ξ )dξ = π n n!δ n,m x = Vx)
More information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 informationEGunGPU
Super Computing in Accelerator simulations - Electron Gun simulation using GPGPU - K. Ohmi, KEK-Accel Accelerator Physics seminar 2009.11.19 Super computers in KEK HITACHI SR11000 POWER5 16 24GB 16 134GFlops,
More informationHigh Melt Strength Polyolefin Elastomers (HMS POEs) and Olefin Block Copolymers (OBCs) Michio ONO* and Takahiko OHMURA(Dow Chemical Japan Ltd, Dow Japan Development Center, 8-1, Ukishimacho, Kawasaki-ku,
More informationCP-PACS CP-PACS CP-PACS : 2048PU+128IOU 614GFLOPS peak 128GByte memory 1058GByte disk 1992 1996 SR2201 : 1996 8 9 CP-PACS Top 500 List ranking No. 1 November 1996 Linpack 368.2Gflops No. 24 Novermber 1999
More information96 7 1m =2 10 7 N 1A 7.1 7.2 a C (1) I (2) A C I A A a A a A A a C C C 7.2: C A C A = = µ 0 2π (1) A C 7.2 AC C A 3 3 µ0 I 2 = 2πa. (2) A C C 7.2 A A
7 Lorentz 7.1 Ampère I 1 I 2 I 2 I 1 L I 1 I 2 21 12 L r 21 = 12 = µ 0 2π I 1 I 2 r L. (7.1) 7.1 µ 0 =4π 10 7 N A 2 (7.2) magnetic permiability I 1 I 2 I 1 I 2 12 21 12 21 7.1: 1m 95 96 7 1m =2 10 7 N
More information1 2 3 4 5 6 0.4% 58.4% 41.2% 10 65 69 12.0% 9 60 64 13.4% 11 70 12.6% 8 55 59 8.6% 0.1% 1 20 24 3.1% 7 50 54 9.3% 2 25 29 6.0% 3 30 34 7.6% 6 45 49 9.7% 4 35 39 8.5% 5 40 44 9.1% 11 70 11.2% 10 65 69 11.0%
More information42 3 u = (37) MeV/c 2 (3.4) [1] u amu m p m n [1] m H [2] m p = (4) MeV/c 2 = (13) u m n = (4) MeV/c 2 =
3 3.1 3.1.1 kg m s J = kg m 2 s 2 MeV MeV [1] 1MeV=1 6 ev = 1.62 176 462 (63) 1 13 J (3.1) [1] 1MeV/c 2 =1.782 661 731 (7) 1 3 kg (3.2) c =1 MeV (atomic mass unit) 12 C u = 1 12 M(12 C) (3.3) 41 42 3 u
More information9 8 7 (x-1.0)*(x-1.0) *(x-1.0) (a) f(a) (b) f(a) Figure 1: f(a) a =1.0 (1) a 1.0 f(1.0)
E-mail: takio-kurita@aist.go.jp 1 ( ) CPU ( ) 2 1. a f(a) =(a 1.0) 2 (1) a ( ) 1(a) f(a) a (1) a f(a) a =2(a 1.0) (2) 2 0 a f(a) a =2(a 1.0) = 0 (3) 1 9 8 7 (x-1.0)*(x-1.0) 6 4 2.0*(x-1.0) 6 2 5 4 0 3-2
More information2 Chapter 4 (f4a). 2. (f4cone) ( θ) () g M. 2. (f4b) T M L P a θ (f4eki) ρ H A a g. v ( ) 2. H(t) ( )
http://astr-www.kj.yamagata-u.ac.jp/~shibata f4a f4b 2 f4cone f4eki f4end 4 f5meanfp f6coin () f6a f7a f7b f7d f8a f8b f9a f9b f9c f9kep f0a f0bt version feqmo fvec4 fvec fvec6 fvec2 fvec3 f3a (-D) f3b
More information003村江.indd
*1 Study on Room ressure Control at Cleanroom art 1 Experiments on Room ressure Fluctuation with Door Operation and Local Ventilation Operation Yukitada MURAE *1 Tamio IWAMURA *2 Hiroyuki NAGAI *3 Shigeru
More information1
GL (a) (b) Ph l P N P h l l Ph Ph Ph Ph l l l l P Ph l P N h l P l .9 αl B βlt D E. 5.5 L r..8 e g s e,e l l W l s l g W W s g l l W W e s g e s g r e l ( s ) l ( l s ) r e l ( s ) l ( l s ) e R e r
More informationHREM Manual37JFAQ
xhrem TM (WinHREM TM /MacHREM TM ) V3.7 !!!!! xhrem Userʼs Guide 2 !!!!!!!!!! Support/Update Email: support@hremresearch.com WEB: www.hremresearch.com xhrem Userʼs Guide 3 ! xhrem Userʼs Guide 4 " " "
More informationJFE.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 information5 H Boltzmann Einstein Brown 5.1 Onsager [ ] Tr Tr Tr = dγ (5.1) A(p, q) Â 0 = Tr Âe βĥ0 Tr e βĥ0 = dγ e βh 0(p,q) A(p, q) dγ e βh 0(p,q) (5.2) e βĥ0
5 H Boltzmann Einstein Brown 5.1 Onsager [ ] Tr Tr Tr = dγ (5.1) A(p, q) Â = Tr Âe βĥ Tr e βĥ = dγ e βh (p,q) A(p, q) dγ e βh (p,q) (5.2) e βĥ A(p, q) p q Â(t) = Tr Â(t)e βĥ Tr e βĥ = dγ() e βĥ(p(),q())
More information1-1 (1) (3) 16.6 6.6 60.9 82.2 32.1 1980 199 1-2 1-3 (2) (2001) 2001 2-1 P A e U ij A ij = e Uij R + e U ij A + e U ij C U ija = a 0 +a 1 c ija +a 2 T ija +a 3 AT ija + Air i Rail Car
More informationt χ 2 F Q t χ 2 F 1 2 µ, σ 2 N(µ, σ 2 ) f(x µ, σ 2 ) = 1 ( exp (x ) µ)2 2πσ 2 2σ 2 0, N(0, 1) (100 α) z(α) t χ 2 *1 2.1 t (i)x N(µ, σ 2 ) x µ σ N(0, 1
t χ F Q t χ F µ, σ N(µ, σ ) f(x µ, σ ) = ( exp (x ) µ) πσ σ 0, N(0, ) (00 α) z(α) t χ *. t (i)x N(µ, σ ) x µ σ N(0, ) (ii)x,, x N(µ, σ ) x = x+ +x N(µ, σ ) (iii) (i),(ii) z = x µ N(0, ) σ N(0, ) ( 9 97.
More information1 filename=mathformula tex 1 ax 2 + bx + c = 0, x = b ± b 2 4ac, (1.1) 2a x 1 + x 2 = b a, x 1x 2 = c a, (1.2) ax 2 + 2b x + c = 0, x = b ± b 2
filename=mathformula58.tex ax + bx + c =, x = b ± b 4ac, (.) a x + x = b a, x x = c a, (.) ax + b x + c =, x = b ± b ac. a (.3). sin(a ± B) = sin A cos B ± cos A sin B, (.) cos(a ± B) = cos A cos B sin
More informationδ ij δ ij ˆx ˆx ŷ ŷ ẑ ẑ 0, ˆx ŷ ŷ ˆx ẑ, ŷ ẑ ẑ ŷ ẑ, ẑ ˆx ˆx ẑ ŷ, a b a x ˆx + a y ŷ + a z ẑ b x ˆx + b
23 2 2.1 n n r x, y, z ˆx ŷ ẑ 1 a a x ˆx + a y ŷ + a z ẑ 2.1.1 3 a iˆx i. 2.1.2 i1 i j k e x e y e z 3 a b a i b i i 1, 2, 3 x y z ˆx i ˆx j δ ij, 2.1.3 n a b a i b i a i b i a x b x + a y b y + a z b
More informationI
I 6 4 10 1 1 1.1............... 1 1................ 1 1.3.................... 1.4............... 1.4.1.............. 1.4................. 1.4.3........... 3 1.4.4.. 3 1.5.......... 3 1.5.1..............
More information( ) I( ) TA: ( M2)
( ) I( ) TA: ( M) 015 7 17 , 7 ( ) I( ).., M. (hatomura@spin.phys.s.u-tokyo.ac.jp).,,.. Keywords: 1. (gas-liquid phase transition). (critical point) 3. (lattice gas model) (Ising model) H = ϕ 0 i,j n i
More informationThe 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 informationLennard Jones Steele * K N nm imac 2015 Mac mini OS *1 N V T
B 2016 4 2 2 1 1.1 Lennard Jones Steele *1 1.2 1.3 1. 2. 3. 4. 77 K N 2 2 2.5 nm imac 2015 Mac mini OS *1 N V T 1.3 3 1.3.1 1. imac 2. physicalchemistry 3. simulation simulation simulation simulation2
More informationIV (2)
COMPUTATIONAL FLUID DYNAMICS (CFD) IV (2) The Analysis of Numerical Schemes (2) 11. Iterative methods for algebraic systems Reima Iwatsu, e-mail : iwatsu@cck.dendai.ac.jp Winter Semester 2007, Graduate
More informationkoji07-02.dvi
007 I II III 1,, 3, 4, 5, 6, 7 5 4 1 ε-n 1 ε-n ε-n ε-n. {a } =1 a ε N N a a N= a a
More information