Observations indicate that reconnection-favored emerging flux has a strong
correlation with coronal mass ejectons (CMEs). Motivated by this observed c
orrelation and based on the flux rope model, an emerging flux trigger mecha
nism is proposed for the onset of CMEs, using two-dimensional magnetohydrod
ynamic (MHD) numerical simulations : when such emerging flux emerges within
the filament channel, it cancels the magnetic field below the flux rope, l
eading to the rise of the flux rope (owing to loss of equilibrium) and the
formation of a current sheet below it. Similar global restructuring and a r
esulting rise motion of the flux rope occur also when reconnection-favored
emerging flux appears on the outer edge of the filament channel. In either
case, fast magnetic reconnection in the current sheet below the flux rope i
nduces fast ejection of the flux rope (i.e., CME). It is also shown that th
e nonreconnecting emerging flux, either within the filament channel or on t
he outer edge of the channel, makes the flux rope move down, i.e., no CMEs
can be triggered. Although the present two-dimensional model can not provid
e many details of the largely unknown three-dimensional processes associate
d with prominence eruptions, it shows some observational features such as t
he height-time profile of erupting prominences. Most importantly, our model
can well explain the observed correlation between CMEs and the reconnectio
n-favored emerging flux.