‘æ121‰ñGMSƒZƒ~ƒi�[

“úŽž�F2024”N2ŒŽ16“ú(‹à)17:15-

�ê�Š�FŠò•ŒŽs�¶ŠUŠw�KƒZƒ“ƒ^�[�E�¬Œ¤�CŽº1

�uŽt�Fûü‹´ ’mŠó Ž��i“Œ‹ž�H‹Æ‘åŠw—�Šw‰@�j

‘è–Ú�FNavier-Stokes flow in the exterior of a moving obstacle with a Lipschitz boundary

ŠT—v�F–³ŒÀ‰“‚Ü‚Å�L‚ª‚é3ŽŸŒ³”ñˆ³�k”S�«—¬‘Ì‚Ì’†‚Å�C‹«ŠE‚ªƒŠƒvƒVƒbƒc˜A‘±‚È�„‘Ì‚ª‰ñ“]‚Æ•À�i‚𔺂¤‰^“®‚ð‚µ‚Ä‚¢‚é‚Æ‚·‚é�D
‚±‚Ì‚Æ‚«�C—¬‘̂̉^“®‚ÍŠO•”ƒŠƒvƒVƒbƒc—̈æ�ã‚ÌNavier-Stokes•û’öŽ®‚É‚æ‚è‹L�q‚³‚ê‚é�D
’è�í‰ð‚̈À’è�«‚Æ‚¢‚Á‚½”ñ�üŒ`–â‘è‚ð‰ð�Í‚·‚é�ã‚Å�C•t��‚·‚锼ŒQ‚Ì L^q-L^r •]‰¿‚ª–{Ž¿“I‚Å‚ ‚è�C�„‘Ì‚ª�ÃŽ~‚µ‚Ä‚¢‚é�ê�‡‚É‚Í�C
Tolksdorf-Watanabe (2020)�CWatanabe (2023)‚É‚æ‚蓱�o‚³‚ê‚Ä‚¢‚é�D
–{�u‰‰‚Å‚Í�C�„‘Ì‚ª‰^“®‚·‚é�ê�‡‚É•t��‚·‚锼ŒQ‚Ì•]‰¿‹y‚Ñ�CNavier-Stokes•û’öŽ®‚ÌŽžŠÔ‘åˆæ‰ð‚ւ̉ž—p‚ɂ‚¢‚Ä�Љ‚é�D
–{�u‰‰‚Í“n粌\ŽsŽ��iŒö—§�z–K“Œ‹ž—�‰È‘åŠw�j‚Æ‚Ì‹¤“¯Œ¤‹†‚ÉŠî‚­�D