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An iterative method for determining the bubble size and bubble oscillation intensity from a record of the acoustic pressure wave emitted by an oscillating bubble is proposed.
The oscillation intensity increases with decreasing immersion depth, increasing inclination of the exit ports, and increasing flow rates.
Increasing oscillation intensity resulted in smaller droplet size due to the increase in both surface shear and surfactant transfer rate to the droplets surface.
Mesoscale OBRs containing helical baffles exhibit wider "operating windows" (i.e. a broader oscillation intensity range) for plug flow than other baffle designs.
A non-linear amplitude is selected to be a universal measure of bubble oscillation intensity and its relation to natural intensity measures is determined.
The analysis reveals interesting facts about vapour bubbles, for which a minimum of the oscillation intensity is found at a certain ambient pressure.
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The emulsion polydispersity decreased with increasing both oscillation intensities as well as dispersed phase flux.
It can be seen that in these experiments the bubble sizes, as defined by the first maximum bubble radius, RM1, ranged from 12.8 to 56.4 mm, and the bubble oscillation intensities, as defined by the non-dimensional peak pressure in the first bubble pulse, pzp1, ranged from 14.3 to 174.
The amplitudes of these oscillation intensities increased with the decrease in phantom size, as did the fluctuations of the reconstructed activity (Figure 3).
The temporal-frequency is the oscillation of intensity against time.
Also the oscillation's intensity is decreased saliently.
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