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A minimum jet velocity is required to initiate desorption.
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It is found that the maximal (centerline) jet velocity first decreases with increasing effective nozzle length, Z = L/(D ⋅ Re), to a minimum at Z∗≈0.0015, beyond which it increases as in developing pipe-flow.
For maximum efficiency the runner tip speed should equal about one-half the striking jet velocity.
First, in order to achieve a high propulsive efficiency, the jet velocity, or the velocity of the gas stream exiting the propulsor, is matched to the flight speed of the aircraft slow aircraft have engines with low jet velocities and fast aircraft have engines with high jet velocities.
V i Jet velocity at impingement, meter per second.
The influences of jet velocity, jet temperature, cooling water velocity and standoff distance are analyzed.
For a jet velocity v ≈ 100 m/s, jet diameters down to 350 nm were found to be feasible.
However, it was weakly dependent on the jet velocity.
It is shown that jet velocity and jet flowrate can be separately specified.
The average jet velocity in each rectangular jet is approximately 5800 cm s−1.
normal jet velocity v n was computed for the 35∘ case of the Ahmed body.
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