レナードジョーンズ(6-12)分子による垂直衝撃波の解析
Contents
1. 0 0 0000000 0 0 dk 124K 3 48x10 mJOOOAOOOOOOOOOOOO OOOO0000000000000000000000000002s80000 0000 0000000000 http www rafal co jp RAFAL 3DQ 000000 2e 021 1e 021 1e 021 INTERMOLECULAR POTENTIAL J o 2e 021 3 5 6 7 8 9 10 INTERMOLECULAR SEPARATION Angstrom 02000000000 642 000 000 0000 1e 010 8e 011 6e 011 4e 011 2e 011 INTERMOLECULAR FORCE N 2e 011 3 5 6 7 8 9 10 INTERMOLECULAR SEPARATION Angstrom 0 3000000000 6120000000000 0000 000000000 000000000 612290 000000000000000000 0000 00 OOOOOO00000000000000000000090000000000000 000 40000 0000 0000000000 http www rafal co jp RAFAL 3DQ 000000 b t4 b 13 e U b 11 b 10 b 9 ARGON g 50m s ARGON g 100m s ARGON g 200m s ARGON g 1000m s ARGON g 3000m s 0 400000000000000000000 12 00000000000000 0000000000000 900000060000 0 Angstrom 000000 00000000000000000000 12 0000000000000000 000 000 oo 1 b x X b 9 r 2 dr m 1 250 ET 3 0000 0000000000 http www rafal co jp RAFAL 3DQ 000000 1 b 12 6 se EIE 0000000000000060000059000 00 0 0 0 OAOOOOOOOO 0000 0 1 00 0 0 0 00 0 0 0000 0000 000 0 200020 020 8e oy ANS b 1 542 2 0 OOOOO0000000000000000000 000000000000000 OO mm00000000000000000000000000 o2. 0000 0000000000 http www rafal co jp RAFAL 3D DO 5 RAFAL 3D DO 5 000000000 12 0000000000000 000 O000000000000000000000 0 00000 DSMCOOOOOOO 000000 00 000 00 0 71 300 0 0 p 0133322Pa0 00000000000000 M 280 OODODOODOOODOODOOOODOODDOAODODOLO m EL ik R Ir Ny I 0 0000000000000 OOOO0000000000000000000000000000 0000 0 0000 0 UU p1 0 133322Pa UU p2 1 273225Pa Tj 300K T 990 3252K 000 n 3 218803x10 m gt 3 gt 1000 n2 9 309830 x 1019m75 p1 2 135201x10 g m OO p2 6 175700x 10 kg m UU Vi 0m s V2 591 0376m s a1 322 5936m s a2 586 1167m s 0000 00 0 000 000 M2 1 00839 00000000 OD V aM 322 5936 x 2 8 903 2621m sD 000 e 0 mo 0 039948 kg mol 00 10000 m 6 633526 x 10 26 kg 0000000000 2 208 1333 J kgK 00 0 y 1 666667 0000 0000000000 http www rafal co jp RAFAL 3D O 1 5 0000000000 00000000000000 632 0 0 0000 wO E 00000000 00 0 0 0 0 0000000000 6 2000 RD e k 124K 3 418 x 10 mJOOOAOOOOOOOOOOOO 0 00 00000000000 ULERETHD A 00000000000000000000 6122 00000000000000 GOO0 000000000000000000000 00000000000 O00000r00 0400000000000000000000000000 000000000000000040000 80000 00000000000 000000000000 632 000000000 0 0 00 O
3. 000000 OOOOOOOODOOO OOO000000000000000000010000 1000000000000 0000 0000 00000000000 OO DOOO0000000000000000000000050000000000 0 000350 00000 OO IMOO0OO000000000000000000060000 250000 000000 0 0 0 001250 O00000 1080000000 00000 QOO0 00 LID 2000000000000000000000000000 el 250000000000 0000000000 H000000000 500000 0 200000000000 21 2200 0 fe PZP Pi O0O0000000000200000 2 05000000000000000 000 OOO0000000000000000 A 0 0549m0 2 2 40000000000 p 0000 0000000000 http www rafal co jp RAFAL 3D 00 5 RAFAL 3D Schmidt 1 O RHO RHO1 RHO2 RHO1 RHO X X LAMBDA1 G 2 0 0 0 0 0 0 00 00 DSMCUHHHHUHHHHHULHUHLHULU 0000000 HP Compaq dc7100SFF pentuim IV 3 6GH2 0 000000 1000 0 1145 0 0 NOOOU 93950000 0 Ll HU 1 Schmidt B Electron beam density measurements in shock waves in argon Jounal of Fluid Mechanics Vol 39 part 2 1969 pp 361 373 2 Hirschfelder J O Curtiss C F and Bird R B Molecular theory of Gases and Liquids John wiley amp sons 1964 p 1110 0000 0000000000 http www rafal co jp RAFAL 3DQ 000000 000000000 12 000000000000 000000 0 0000000 6 12 0 0000 0 00000000000 90 00 12 ox on Y 0 000000000000000 6 12 000000000 e000000 0 D10000000000000000 r c0000000 ro 2 8 1 1224620 0000 eq n m o r 01000000000 642 0 0000000 0000 MOLA re TOO 0000 000000000 6000 0
4. O CI cl 0 aa or 2 7 x 8 x 3 418 x 10719 2 348951 x 10717 m 0000000000000 070 DSMCO0000000000000000000 OOOO00000000000000000000000000000000000 00000000000000 OOO00000000030 1 A Vo OOODODOOODUOOOLUea UODOOOODODOOODODOTOODUODOUODOO 0000 orUNUNUUNUNU mUnULLLLU l V2 x 2 348951 x 10 17 x 9 309830 x 1019 unun 200000 7 00 0 0 0 0 710 3 233347 x 1071 m Ty Or gt 0000000000 0000000000000000 m SRT C Re T 000000 0000 0000000000 http www rafal co jp RAFAL 3D 1 5 OOOOTODODOODDODODDOO 7 990 3252K 0 0 0 DO ii VE x 208 1333 x 990 3252 T 724 4856 m s 0000 00000000000 70 3 233347 x 1074 co 724 4856 4 462618 x 1077 s 0000 DSMCJ 000000 2000000000000000 000000000 U 2000 000 15m0 y0 OO 0 006mOODOODOODOADOODOODOO TOO 750000 00 10000 75000 2mmx5nnJQJO0000000 0 005m 1 5m 020000 000000000 OD DD 20000000000000000000000000000000000 OOOO00000000000000000000000000000830000 MAT T 300K p 0 133322Pa OU 300 100000 OO WO 2000000000000000000000000000000000 OOOO00000000000000040000 0000 0000000000 http www rafal co jp RAFAL 3D 00 5 MAB MAB T1 300K 12 990 3252K P1 0 133322Pa P2 1 273225Pa V1 0m s V2 591 0376m s Bura SCN REGER 0 400 900000 0000000 At At 6x10 J0000000000000000007001 740000000 7244856m s 0 000 0 002m0 000000 1460
5. bitng 00 00 0SOOOOO9000000000000x000000000000000000 0000000000000 0 4000000000000000000000000 0000 DEFLECTION ANGLE DEG DEFLECTION ANGLE DEG 0 2 4 6 8 10 12 14 16 0 2 4 6 8 10 12 14 16 IMPACT PARAMETER Angstrom IMPACT PARAMETER Angstrom 1 g 50m s g 100m s DEFLECTION ANGLE DEG DEFLECTION ANGLE DEG a 0 2 4 6 8 10 12 14 16 o 2 4 6 8 10 12 14 16 18 IMPACT PARAMETER Angstrom IMPACT PARAMETER Angstrom 1 g 200m s g 400m s 0 5 100000000000G00000 00000000000 0000 0000000000 http www rafal co jp RAFAL 3D 00000 DEFLECTION ANGLE DEG 0 2 4 6 8 10 12 14 IMPACT PARAMETER Angstrom g 1000m s 16 18 DEFLECTION ANGLE DEG 180 160 140 120 100 80 60 40 20 20 0 2 4 6 8 10 12 14 16 18 IMPACT PARAMETER Angstrom g 3000m s 0 5 200000000000 000000 00000000000 000 1 Hirschfelder J O Curtiss C F and Bird R B Molecular theory of Gases and Liquids John wiley amp sons 1964 p 1110
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