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The changeover occurs at the critical concentration gradient corresponding to peak propagation velocity.
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Juxtaposition of the crack velocity with this spacing suggests that the crack takes ∼10−10 s for peak-to-peak propagation.
With the increase of spraying time of water mist and fraction of nitrogen, the initial shape of the explosion flame became snakelike, and at the same time the peak flame propagation speed and peak overpressure decreased significantly.
This leads to a trade-off between two effects: (i) Multipath increases the signal diversity and thus creates peaks in the CCF that better represent the true distance, but (ii) multipath also generates "wrong" (additional) peaks from propagation paths that do not directly travel through the receivers, which in turn reduce the accuracy of distance estimation.
The bifurcated heat release rate peak exhibited negative propagation speed relative to the local flow velocity by consuming a separated methane/air mixture in the downstream side of the boundary zone between an incoming fresh mixture and burned gas.
The main and two bifurcated peaks exhibited negative propagation speeds relative to local flow velocity by consuming the remaining intermediates.
Large-scale circular waves with two negative peaks, a large propagation velocity (3,457 m/s and 783 m/s), and strong dissipation (travelling distance is about 1,000 km) propagated in a radial direction from 06:00 UT to 06:15 UT.
First, a group of resonance peaks within a propagation band can be reduced in level by using only one neutralizer, the number reduced depending on the number of bays and the location.
The averaged peak pressure of back-propagation pressure waves in the air plenum chamber was discussed.
The averaged peak pressure of back-propagation pressure waves in the air plenum chamber had the same change trend under multi-tube firing patterns.
Some exotic cases are presented including oblique propagation, station position under the peak height etc. Peak height global distribution is described as well as neutral wind parameters derived from the topside peak height values.
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