Proceedings of the International School of Physics "Enrico Fermi.", Volume 65N. Zanichelli, 1978 - Nuclear physics |
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Page 837
Equation ( 10 ) shows that , starting from mi > mo , mass loss from the primary
results in a decrease of a , until mı = mg . After this , further mass loss from the
primary results in an increase of a . Since , for decreasing mi / m2 , also ry
decreases ...
Equation ( 10 ) shows that , starting from mi > mo , mass loss from the primary
results in a decrease of a , until mı = mg . After this , further mass loss from the
primary results in an increase of a . Since , for decreasing mi / m2 , also ry
decreases ...
Page 838
The variation of the thermal - equilibrium radius of the primary component Rı and
the radius of its Roche lobe r , during the mass transfer from primary to secondary
. Only after the roles of primary and secondary have been reversed will r ...
The variation of the thermal - equilibrium radius of the primary component Rı and
the radius of its Roche lobe r , during the mass transfer from primary to secondary
. Only after the roles of primary and secondary have been reversed will r ...
Page 839
Then , for « low - mass » systems [ 32 , 33 ) , the primary has become an
overluminous subgiant in the shell hydrogen - burning stage ( with a degenerate
helium core ) . The envelope continues to expand on a nuclear time scale and
slow ...
Then , for « low - mass » systems [ 32 , 33 ) , the primary has become an
overluminous subgiant in the shell hydrogen - burning stage ( with a degenerate
helium core ) . The envelope continues to expand on a nuclear time scale and
slow ...
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Contents
Gruppo fotografico del partecipanti al Corso | 1 |
Introduction | 17 |
Сen | 37 |
Copyright | |
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