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Variations in room temperature during mixing leads to at most (Formula presented) Torr uncertainty in the total dissolved noble-gas pressure. This uncertainty does not affect the qualitative variation of light intensity as a function of mixture ratio shown in Fig. 33
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Variations in room temperature during mixing leads to at most (Formula presented) Torr uncertainty in the total dissolved noble-gas pressure. This uncertainty does not affect the qualitative variation of light intensity as a function of mixture ratio shown in Fig. 33.
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D.F. Gaitan, Ph. D. thesis, University of Mississippi, 1990 (unpublished)
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M. Honevac, software package LightLab: Far Field Mie Scattering (Valley Scientific, Valley City, OH, 1998).
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A dynamic diffusive equilibrium is independently established between each constituent noble gas in the bubble and that dissolved in water. The segregation is likely to take place over a short time compared to the acoustic period and it does not affect this diffusive equilibrium 4. It is then reasonable that the mixture fraction as applied during the mixing procedure is the mixture fraction in the bubble itself. In evaluating x, the differences in the diffusivity and solubility of different noble-gas species do not enter. Since the total noble-gas content is kept constant at 1% of the total dissolved gas, the (Formula presented) relation is the same for all mixtures in agreement with our observation
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A dynamic diffusive equilibrium is independently established between each constituent noble gas in the bubble and that dissolved in water. The segregation is likely to take place over a short time compared to the acoustic period and it does not affect this diffusive equilibrium 4. It is then reasonable that the mixture fraction as applied during the mixing procedure is the mixture fraction in the bubble itself. In evaluating x, the differences in the diffusivity and solubility of different noble-gas species do not enter. Since the total noble-gas content is kept constant at 1% of the total dissolved gas, the (Formula presented) relation is the same for all mixtures in agreement with our observation.
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19
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The entire acoustic apparatus was reassembled between the two sets of measurements (a) and (b) in Fig. 33. The reassembly is the likely cause for the systematic difference in the data of “pure” He in the two datasets
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The entire acoustic apparatus was reassembled between the two sets of measurements (a) and (b) in Fig. 33. The reassembly is the likely cause for the systematic difference in the data of “pure” He in the two datasets.
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