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Do the particles follow the flow?


In section 2.2, I derived a comparison that can be used to test whether the particles follow the flow. The kinematic viscosity of the water-glycerol mixture, that is the bulk of the film, can be found in table 3.3. If the smallest particle radius, tex2html_wrap_inline4597, is inserted as the particle radius in equation 2.6 and the energy dissipation is separated out we get an upper bound for the energy dissipation as the condition for the particles to follow the flow of the soap film:
When the largest particle radius, tex2html_wrap_inline4599, is inserted the condition is:

The energy dissipation can be found by comparing the mechanical energy (potential plus kinetic) of the film at two locations along the channel. The mechanical energy per unit mass is
where g denotes the gravitational acceleration, h denotes the height, and v denotes the velocity. The time it takes to flow a stretch l along the channel is
if the velocity does not change much. I let the subscripts 1 and 2 denote values at two locations along the channel separated by a distance l. The energy dissipation is the mechanical energy per unit mass per unit time that disappears from the system:

At two cross sections separated tex2html_wrap_inline4615 along the channel I find that the mean square velocity is tex2html_wrap_inline4617 (upstream) and tex2html_wrap_inline4619 (downstream). The inclination is tex2html_wrap_inline4589, and the gravitational acceleration is tex2html_wrap_inline4623. If we insert these values in expression 3.5 we find
This number is rather high compared to the magnitude of the energy dissipation you usually find in three-dimensional turbulence (tex2html_wrap_inline4625 in wind tunnels), so I suspect that there is something wrong either in my derivation, or in my velocity measurementsgif.

The energy dissipation in the soap film is (apparently) larger than what can be tolerated, if the largest particles I have poured on to the soap film should follow the flow of the soap film. Since the largest particles are those that are visible on the images, this means that the value of this collection of measurements is limited.

If we rewrite equation 2.6 so it expresses a limit on the particle radius and insert the tabular value for the kinematic viscosity and the value for the energy dissipation from the preceding derivation we get
If we could separate the smallest particles from the mixture of particles of various sizes, and just use them as tracers, we would have some tracers that would follow the flow.

next up previous contents index
Next: Data processing Up: Soap Film Experiment Previous: Creating a running soap