The instability of the surface of discontinuity separating two streams
of immiscible constant-density fluids is studied experimentally and t
heoretically near onset when surface tension effects are significant.
Following Thorpe's original idea, a tube filled with two immiscible fl
uids is tilted at an angle and returned to its horizontal position to
produce a nearly constant velocity difference between both streams tha
t can be varied continuously across threshold. In order to control the
wavenumber near onset, the flow is spatially forced by periodically d
istributing small obstacles on the upper side of the tank. When the ki
nematic viscosities of each fluid are nearly equal, ones observes two
counter-propagating waves of equal amplitude, which cannot be explaine
d from a vortex sheet model. A linear stability analysis of a density
discontinuity embedded within a piecewise-linear velocity profile demo
nstrates that such waves are Holmboe modes associated with the diffusi
ve layers above and below the interface. Good agreement is obtained be
tween the measured and predicted values of the critical velocity diffe
rence, propagation velocity and growth factors of the waves. The insta
bility analysis of the asymmetric velocity profile reveals that the br
eaking of reflectional symmetry gives rise to a single propagating wav
e near onset. When the kinematic viscosities of each fluid differ, the
first destabilized wave is observed to propagate in the same directio
n as the less-viscous fluid, in agreement with the theoretical results
, and the dominant direction of propagation can be manipulated by adju
sting the viscosities accordingly.