{"schema":"pubphys.bundle/1","record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.revision/1","content_sha256":"d05c8374ea90efe0b25af44caa86ec02d6164e516e8063d8d90374dd5a2772cd","created":"2026-10-03T07:18:04Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":["5475cf5dc5b1a72283d26dc95dc6e00d7ea4e00096a7c6492e409a1816eeb011"],"salt":"3146e0b749d261f361678e812e0007f65b7a7d1e8c9e1bd0146fc59edf76feec","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"revision"},"content":{"answer_type":"yes-no","assisted_by":[],"external_id":"fluid.rb-convection.ultimate-existence","kind":"well-posed","literature_status":"contested","n":"1","parents":[],"plain":"When heating from below is strong enough, theory predicts that heat transport should grow as the square root of the heating strength, much faster than at moderate heating. Laboratories using different fluids and cells disagree on whether this 'ultimate' regime has been observed.","posed_since":"1962","precise":"System: Oberbeck-Boussinesq Rayleigh-Benard convection between smooth isothermal no-slip plates, Prandtl number $\\mathrm{Pr} \\sim 1$, aspect ratio $\\Gamma \\sim 1$. Quantity: Nusselt number $\\mathrm{Nu}(\\mathrm{Ra})$ as $\\mathrm{Ra} \\to \\infty$. Question: does the effective exponent gamma = d ln Nu / d ln Ra cross over from about $1/3$ to the Kraichnan form Nu ~ Ra^(1/2) (ln Ra)^(-c) at finite Ra, or does $\\mathrm{Nu} \\sim \\mathrm{Ra}^{1/3}$ persist? Answer: $\\gamma(\\mathrm{Ra})$ up to $\\mathrm{Ra} \\sim 10^{17}$ with non-Boussinesq, sidewall and plate corrections quantified.","problem_ref":null,"references":"","settled_by":"Concordant heat-transport measurements in at least two independent cells at $Ra>10^{15}$ with full uncertainty analysis, supported by DNS reaching $Ra\\sim 10^{16}$.","status_note":"Gottingen SF6 data show a transition between $\\mathrm{Ra} \\sim 10^{13} \\text{ and } 5 x 10^{14}$ (He et al. 2012) and Grenoble helium data near $10^{11}$ (Chavanne et al. 1997), Oregon and Brno helium data do not; slender-cell DNS give $\\gamma \\sim 0.33$ up to $\\mathrm{Ra} \\sim 10^{15}$ (Iyer et al. 2020); a 2026 Brno uncertainty analysis shows data corrections can decide the claim (Urban et al., arXiv:2603.08811).","title":"Does the ultimate $\\mathrm{Nu} \\sim \\mathrm{Ra}^{1/2}$ regime exist in Rayleigh-Benard convection?","topic_ref":"6d62b34c8e014f88ffcbe79c7a106852a6fbdddb7610842d4118538cb9b5370d"},"content_withheld":"false","files":[],"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"e63ee327747bcfad2d5d8e990f17a84cadc6fa47142aa9b3f0c612a01fa2862d","schema":"pubphys.attested/1"},"id_token":null,"id_token_withheld":"false","envelope":{"attested_hash":"8fbe7570b6c5374f5ced8298370949898f890828e3347898eaf4c5df56344464","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"A8WEemcFVc_Ekqv3HCTcWQIgCCU__-FMx1w2BhqjZ_vHqyu8VO7dml7XEZIE3wqf8TwhNXTAl_FLrQo-yHUzBw"},"schema":"pubphys.envelope/1"},"ots":{"attested":["AE9wZW5UaW1lc3RhbXBzAABQcm9vZgC_ieLohOiSlAEIj751cLbFN09c7YKYNwlJiY-JCCjjNHiY6vTF31Y0RGTwII_BqvVesQy0LqWu88t5afpoTtgw475uJ3D7svV5Vh1ECPEgQBnJjxgfrkIYRdyN-uB9b6JtASEPMQk03mlZT-MGZIQI8SCSIlIjVAg48jeSUmiTlwZq6TBkHI9ODzTMprjNy6yH0QjxIDyVIeG1tSkmTG8kCnHifEzEXVR0AtHBcVB3iYFjYMVVCPAgvL_0vBiZcOhX0fO7fkxiWDwQ5KlAt4fdOt6yTLPp1h8I8SC2ncMk6p_HRHs0Bwy46VSQqmQQrEdB7-arJkD95-n-RwjwIBuXyrcwi8vWjA4uFLMsDvI7QxQ03VAxIfMd0CQI4GySCPAgyYYKAjmHpniaTNWfQfwaMNMI3Vm3FjqZ7JUny3t_J48I8SAzYkfrMCtnlPZF7RCs0vhySIZDq30HHv5Q-Y2E93F_lgjwIIhzmnVeFxVHRiBmi7SsQd_gIBRvsrzzZf-fzyEkp8wnCPAgy6DmLQtIuWm-zrDRmaSy95vcFWsjvWyppQO7wIWrfC4I8SAQuuTPkAGyvS_wKMy9BtKvnki2puESdY2vXem8hT1uIQjwIBGYo5Vxy-d7U5zKv5vp3Ii7hJPH_BDLCzA13c47p9q7CP_wCHbghVgOFMuNCPAQPZK2lHbTMqcCYUotzOQcmQjwIJ7ruRIs6HnufKxCpmLUgeUl0aUu0ov4_3PqcppS-bddCPEgI530vHzdwz_3o9jYQ3WablSaV64Wfn7Pmby5WLyI-A0I8QRqwKw78AhITF7Tr3a1xP8Ag9_jDS75DI4sK2h0dHBzOi8vYm9iLmJ0Yy5jYWxlbmRhci5vcGVudGltZXN0YW1wcy5vcmcI8CBXWeNiWFWltfHE0nkDXsVKIykUUwuObhsnN-2fvBt98gjwIM5Vf7j68sOFgVysYMc5S09Hho-fqxYW3oQ4oKUX7JpPCPAgaKHHQB3sdd9w1hu4NMh7vmb-p0X2r4uyVKKCj1G7S28I8SAW2Mg6Bzi9ygjrrjIYB7w90fwMcxH24SsqLmzPyAMGfwjwIMQ863zlveYIpNKWVrZaDOa4vowwoOg2CcTW8gXtxK3dCPEgrZxGGAf-t8jhz_eLMUyBN1IhNrdYDRcNHWvQcwNG9woI8CCVOUHG1YXudbaFIgUYvrCIevRWvb2ubhQAo-z0duD0rQjxIDBeKerVGkO3J2eXDwdraSioXbIWsdIPEN1s8pIwJIS2CPAgV2kB3n3JZ5HwBQjpRL1CWKnqvdCjZk3RcALk6N2wHigI8CB-wbljNlfqElD25uZkNg6taS81YDRU2vfMqGVQ420O9AjxWQEAAAABJM43UU6MLMRrPlCUqossvu1q_knons5yylyWTgxZzWUAAAAAAP7___8CLgABAAAAAAAWABQrYt3E7OllKRCEmL3FL589l78_5wAAAAAAAAAAImog8ATiyw4ACAjxILmbcIO7ixv3pCtwUMZ1VQGKus54F9lZ8-w5ECD5ZuiICAjwIG6ynCyFTLPE7Rgk-0ZGCtBDyqNQx8YvaSZNHy8D8p8jCAjwIMX8zoD2Be1YWvcx_bexVPRmBX0hK-do8b8t9SarimQVCAjxIG6XtpqIEclLlhzcK1LVjqoPGrjjmLnyno8tcETMzECECAjwIF6mlfXOFY51JhrK4eze8zQlKV75OYZYqbtyi8BWxmAsCAjwIKKUcJmVoz-u-geiRV_-ZHdF0VEPXaEPFWf_JX_0e7G2CAjxIGMeD0Z5QWNKBcAEpHht007FFIILW6aSJ8f3CMkKNsneCAjwIBFr6Je8rkB7kwhPGbq0yRgFwZsvW9JhY5sXDRtrq0QwCAjwIAHAwXaus-yUgKICJB5mVvx8VZuJgjwnpb0qWPg1pi6DCAjxIAJhb8cefkVHTAMymdsxa-_i-tUua62LcpALQnPG7R9_CAjwIDvsFqBhPfAL6TCtXZd7gBWmMpx6iiZ-Ug0Jf_LlcstgCAjwIDJRBX6Q0Vge-ra-k1_g76yJWTEp6WWF13I3JpTnsZPJCAjwILykZCbkC9VQgl5gytPKKir6T9nTvKR6y05iWSHBTQgzCAgABYiWDXPXGQED45c78Ah-sGbmQAwfZwjwEAYqxtHnZiPZnJEGPx_JvKsI8SDXkqDg17YsZIrEz5acRx7mBXCKW5mKNgRYnw_-U2cpDgjxBGrArDrwCEfK6Mono428_wCD3-MNLvkMji4taHR0cHM6Ly9hbGljZS5idGMuY2FsZW5kYXIub3BlbnRpbWVzdGFtcHMub3JnCPAg10nyJ6Jn4kshQQQCKE0Lvj3hBC6nLRBVIzaPV4eh8VwI8CCQaAqWlxEbac_XOq1MOlf9iOKHEsxXspzbjK0vLpy8BwjwII3iRbRXUcDxrhAdkZmFlI15nySCSEZ7g922tF1Xln5DCPEgYYvZ1L4v4rPu_UqLfcHPtwSb2OH2GhPgVcVhhH6DpkQI8CDZCIoR20sC-uchP40oAmcLm9EJFV7xzwplj54AeVadXQjxILvLBjPFpCoz29m9Yf2qRnV7PI9GqxE8ozVQfk9QwCqrCPEgZXcMudvEoB_MJ8tqOW2PLTKAIeQBnE-1bfzptRc2gR8I8VkBAAAAAfXq-bmxWqOz7B5wKkwjzHGv2R4s7Y0Z76LqXWYNhmz0AAAAAAD-____Av0cAAAAAAAAFgAUl-skmdZDtn7Hnub6mF4HP2uVn7oAAAAAAAAAACJqIPAE4MsOAAgI8CBDmQsbEXc46Hu8DivhCBM1LGExa4TTM-wo7HpoCVjBTQgI8CCty5vkQtPHzzs8xqArOYhVSjgaDoG1ou3cojv5_P7wQQgI8SDQWB0kdXCTwbk-TqTt0QfRMyzDNLOtU1XXFgvGSRlW8wgI8CC2PKa_QCIBZtrXodq1GdEzppISMsMRDOnzr2gFjLKOAAgI8CCwQ_QF67bcFk_uJ2s0VCZmf5PGIjTmTCpt_qnVY5p_8AgI8SAbzyx7z-oxPMju6PvtQhzrJIQyH2ZAc9oyLuYemzbmZQgI8CC5bh7J74uUk91r8LwybHQFCNBC3PWeuwtMCCNFKWj19AgI8SAf4R2TUNPjaX_PWDUImpoITK0JoW89zaMKnD1wlEEi8AgI8SC2vNmdm7eyP5Ytl1yTzT0njliMdALl1ViKG-s3bG2zswgI8CCpbIVNz1GFVXdJk2zd82hBUoNFFemUPBt7IJdWEOciPwgI8CBtYdRQcrtX1FtCm1SxF7sx-5cO04U8KzbJh8fqBkyReAgI8CBHs2LGmX6gI-lV7yp1RrV7_tGfdiBAwnEFF6B6yXHzAQgI8CATotVmbXBMAixhZ-QKy5Q4lR0FusdA_wcIC1TbB7GmxAgIAAWIlg1z1xkBA-KXOw"],"envelope":["AE9wZW5UaW1lc3RhbXBzAABQcm9vZgC_ieLohOiSlAEIneimhiy26_y-NUDLfUsAn4kS_Ak-7XHWc_Nk6dpu5UzwIJ3r60CdFZGbFK3PcJWf9ZQRRDB6TUXO85yEyk93y7iaCPAgxC6DtDPqJ3nTq2SfV_MTpB5_sqZRWp9V6yucLGnJvrgI8SBjD_j5pAhNcrWr4-fSaeUjINdHELWrS_35Iy3iHDMIRgjwIP9MDEoBV83q9gohjFDWLiKFVFsz4pZ8RhhBWTttFf9CCPAgRXN-bWRFBKB-h8Y84c6AFSeA--IenLf_LzWcNqxZWOoI8SDWTVc8Knw2O1OG69vy8YEwJplSUfSLCnx7lyJlmAtjeQjwIFOuMtkA1LNDpwHC6veKLJYyL459iDJzE8koE8xHbrjhCPAgwmK3CUEOY-5QE2iSOuU3W3YgTzeiLK0zofehysSfjssI8CB0Pk63gwyd_u5K2K1drJW3UxU3mXTBkDKQdutj6_nnEgjxIFf8EhaVa-ubjpYx3wEAcKGxkzfUQq6B-8jimpRd8IqnCPAgy6DmLQtIuWm-zrDRmaSy95vcFWsjvWyppQO7wIWrfC4I8SAQuuTPkAGyvS_wKMy9BtKvnki2puESdY2vXem8hT1uIQjwIBGYo5Vxy-d7U5zKv5vp3Ii7hJPH_BDLCzA13c47p9q7CP_wCHbghVgOFMuNCPAQPZK2lHbTMqcCYUotzOQcmQjwIJ7ruRIs6HnufKxCpmLUgeUl0aUu0ov4_3PqcppS-bddCPEgI530vHzdwz_3o9jYQ3WablSa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