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For a given agglomerate, there was a threshold velocity, above which would increase aerosolisation and otherwise would decrease.
The results show a reduction of 30% of the cage volume for current velocity above 0.6 m/s.
When increasing the cross-flow velocity above 0.24 m/s a plateau in permeate flux was observed.
With increasing hot zone velocity above 30 mm/h, the columnar grains became narrower.
Thus, the shattering efficiency is the largest for the smallest grains that attain a velocity above the shattering threshold.
This discrepancy may result from a trade-off between the depth of a reflector and velocity above the reflector.
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The effective conduction velocities determined above are the consequence of both the magnitude, and the direction, θ, of AP conduction through the MEA.
Enormous amounts of masonry, glass, wood, metal, and other debris created by the initial shock wave will fly at velocities above 160 km (100 miles) per hour, causing further destruction.
The most severe fracture patterns were elicited by velocities above 3.5 m/s.
Accurate agreement between experimental results and predicted curves was found for gas velocities above a critical velocity, quantified as 1·5 ms−1·5
Fragmentation at velocities above the critical velocity is not well reproduced due to excessive element erosion.
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