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We will consider surface tension as the only driving mechanism.
The current concern is with two main aspects, namely surface tension and post-impact phenomena.
In both cases, there was premature foaming, lowered surface tension and elevated rhamnolipid levels.
We outline the theory for the former, in the case where surface tension effects at the moving boundary are ignored.
The relative surface tension is m = 0.5 and therefore /6 = 0.083.
This solution is analysed in the limit of small surface tension.
Five separate readings of surface tension were taken during each experiment and an average value obtained.
We have already noted the marked effect, shown in figures 4, 10, and 15, of differing viscosities in the absence of surface tension.
With finite surface tension, we observed the onset of numerical instabilities of the sawtooth type.
However, a t this value of surface tension, there is no dimpling of the rising drop.
The fluid is assumed to be ideal and surface tension is ignored.
As in the previous section, we have investigated the effect of surface tension on a single case.
They find by perturbing about infinite adsorption rate that there is a decrease in the film thickness due to surface tension gradient.
The non-uniqueness in case 3 is not avoided by taking surface tension into consideration.
The spreading on a water-air interface of a thin liquid film is examined for the situation in which surface tension gradients drive the motion.
