By substituting, we have obtained a solution for c in terms of known variables. Note that
, which is arbitrary, is multiplying every term linearly and will cancel.
![[Graphics:../Images/linstab_gr_136.gif]](../Images/linstab_gr_136.gif)
This can be written more concisely as
![[Graphics:../Images/linstab_gr_138.gif]](../Images/linstab_gr_138.gif)
This is the dispersion relation for the wave speed.
The solutions are:
![[Graphics:../Images/linstab_gr_140.gif]](../Images/linstab_gr_140.gif)
![[Graphics:../Images/linstab_gr_141.gif]](../Images/linstab_gr_141.gif)
Which should be a set of upstream and downstream traveling waves.
c1 will be the upstream wave and will not appear in a flow system
c2 will be the downstream wave that we would like to study the behavior of
![[Graphics:../Images/linstab_gr_143.gif]](../Images/linstab_gr_143.gif)
![[Graphics:../Images/linstab_gr_145.gif]](../Images/linstab_gr_145.gif)