可触知
发表于 2025-3-25 07:12:24
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有权威
发表于 2025-3-25 10:29:34
Sonic Point Instability and Stochastic Excitation of Oscillations by Turbulencease of relativistic disks, the accretion flows fall to central objects by passing a sonic point. In the case where the sonic point is a nodal-type critical point, accretion flows are locally unstable at the sonic point and waves propagating both inward and outward are generated there. This is an int
foliage
发表于 2025-3-25 11:41:41
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善辩
发表于 2025-3-25 16:57:23
range of effective temperatures from 14 200 K down to 11400 K. Comparison with mixing length theory (MLT) yields a conflicting picture: The dynamics of convection is not governed by up- and downflowing bubbles which dissolve after travelling some characteristic distance - but by the formation, advec
无能的人
发表于 2025-3-25 23:35:18
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概观
发表于 2025-3-26 02:01:21
Shoji Katorange of effective temperatures from 14 200 K down to 11400 K. Comparison with mixing length theory (MLT) yields a conflicting picture: The dynamics of convection is not governed by up- and downflowing bubbles which dissolve after travelling some characteristic distance - but by the formation, advec
射手座
发表于 2025-3-26 05:05:37
Shoji Katorange of effective temperatures from 14 200 K down to 11400 K. Comparison with mixing length theory (MLT) yields a conflicting picture: The dynamics of convection is not governed by up- and downflowing bubbles which dissolve after travelling some characteristic distance - but by the formation, advec
Amylase
发表于 2025-3-26 10:13:02
Shoji Katorange of effective temperatures from 14 200 K down to 11400 K. Comparison with mixing length theory (MLT) yields a conflicting picture: The dynamics of convection is not governed by up- and downflowing bubbles which dissolve after travelling some characteristic distance - but by the formation, advec
伴随而来
发表于 2025-3-26 13:40:48
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Polydipsia
发表于 2025-3-26 19:13:24
Shoji Katorange of effective temperatures from 14 200 K down to 11400 K. Comparison with mixing length theory (MLT) yields a conflicting picture: The dynamics of convection is not governed by up- and downflowing bubbles which dissolve after travelling some characteristic distance - but by the formation, advec