逢甲學報, Band 13逢甲大學, 1980 |
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... constant , the displacement tends to damp out quickly . This result is anticipated . As q increa- ses with a and k remaining unchanged , the displacement tends to approach the state of sustained oscillations and further increase of q ...
... constant , the displacement tends to damp out quickly . This result is anticipated . As q increa- ses with a and k remaining unchanged , the displacement tends to approach the state of sustained oscillations and further increase of q ...
Seite
... constant . Therefore and dC ′ ( t ) = C ' ( t ) [ — B — iS ] dt C ' ( t ) = exp { ( B - iS ) t } . The line profile can thus be evaluated : I ( w ) = x 1 Re√√00 elot C ( t ) dt B / ( w - w 。- S ) 2 + B2 2 where Re { } denotes " the ...
... constant . Therefore and dC ′ ( t ) = C ' ( t ) [ — B — iS ] dt C ' ( t ) = exp { ( B - iS ) t } . The line profile can thus be evaluated : I ( w ) = x 1 Re√√00 elot C ( t ) dt B / ( w - w 。- S ) 2 + B2 2 where Re { } denotes " the ...
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... constant . Therefore dC ' ( t ) = C ′ ( t ) [ — B - iS ] dt and C ' ( t ) = exp ( -B - is ) t } . The line profile can thus be evaluated : 1 I ( w ) = = Re 元 elot C ( t ) dt 0 B / ( w - w 。- S ) 2 + B2 where Re { } denotes " the real ...
... constant . Therefore dC ' ( t ) = C ′ ( t ) [ — B - iS ] dt and C ' ( t ) = exp ( -B - is ) t } . The line profile can thus be evaluated : 1 I ( w ) = = Re 元 elot C ( t ) dt 0 B / ( w - w 。- S ) 2 + B2 where Re { } denotes " the real ...