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Liquids analysis temperature variations effect

The approximate analysis of Nusselt has been applied to a wide variety of geometries. Common assumptions include uniform wall temperature, saturated and quiescent vapor, no interfacial resistance at the liquid-vapor interface, no momentum and convection effects in the condensate, and no variation of properties with temperature. The resulting equations are valid for ordinary liquids (i.e., nonliquid metals) provided (cpeATIi(g) is less than about 0.2 to 0.5. [Pg.951]

See other pages where Liquids analysis temperature variations effect is mentioned: [Pg.22]    [Pg.23]    [Pg.21]    [Pg.167]    [Pg.301]    [Pg.123]    [Pg.405]    [Pg.1958]    [Pg.730]    [Pg.695]    [Pg.171]    [Pg.46]    [Pg.195]    [Pg.41]    [Pg.154]    [Pg.181]    [Pg.248]    [Pg.81]    [Pg.21]    [Pg.28]    [Pg.164]    [Pg.213]    [Pg.127]    [Pg.440]    [Pg.155]    [Pg.1096]    [Pg.341]    [Pg.113]    [Pg.441]    [Pg.269]    [Pg.715]    [Pg.198]    [Pg.122]    [Pg.90]    [Pg.96]    [Pg.978]    [Pg.7094]    [Pg.8275]    [Pg.178]    [Pg.154]    [Pg.254]    [Pg.214]    [Pg.665]    [Pg.412]    [Pg.90]    [Pg.968]   
See also in sourсe #XX -- [ Pg.729 , Pg.730 ]



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