... B t . EquJ2000.0 . NGC4559 . 12 35 57.7 . +27 57 35 . 814 . 10.30 . ... EquJ2000.0 . NGC4559 . 12 35 57.7 . +27 57 35 . 814 . 10.30 . SDSS . ... a Holm . b/a . A B G . m FUV . B T . m H . K s . ...
... Cas1 . 02 06 07.9 . +69 00 36 . 35 . 15.30 . DSS-2 J . Object Names . ... a Holm . b/a . A B G . m FUV . B T . m H . K s . ... A B G . m FUV . B T . m H . K s . m 21 . W 50 . ...
... B t . EquJ2000.0 . Cas III . 00 35 59.4 . +51 33 35 . -372 . 13.70 . ... EquJ2000.0 . Cas III . 00 35 59.4 . +51 33 35 . -372 . 13.70 . DSS-2 B . ... a Holm . b/a . A B G . m FUV . B T . m H . K s . ...
... Correspondingly, for the potential and the force o f attraction around 'the point' wit h the rest mass equal to M in the space wit h r>> GM/c2 we must have formulae (29) and (35) fro m [PI], i.e., Newton's law. ...
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Ссылки http://mavr.sao.ru/hq/grb/team/vvs/03_Properties_strong_field.pdf -- 963.3 Кб -- 30.12.2010 Похожие документы
... B t . EquJ2000.0 . DDO194 . 14 35 24.6 . +57 15 24 . 218 . 14.50 . ... a Holm . b/a . A B G . m FUV . B T . m H . K s . ... A B G . m FUV . B T . m H . K s . m 21 . W 50 . ...