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When the field is applied against the direction of front propagation ("negative" field), wave saturation is obtained, characterized by a slight increase in the velocity of propagation with field strength, until it reaches a constant value as the field strength is further increased.
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Later tests used a variety of propagations, either 0.5 or 0.9, in order to simulate the propagation of negative information across the network.
The distribution tree is split into many stubs to limit the maximum number of hop-counts in each distribution tree; a small number of hop-counts suppresses propagation of negative effects, including disconnections and delay jitters [14].
Nodes with higher estimated relay ability are located at more upstream positions in the trees, while nodes with lower estimated relay ability are positioned downstream to avoid the propagation of negative effects.
Across a network of papers, however, the barrier to the propagation of negative results biases claims as being viewed as true until proved false.
It is found that while the fluid normal straining is positive and tends to separate iso-scalar surfaces, the dominating normal strain rate due to self-propagation is negative and tends to bring the iso-scalar surfaces closer resulting in overall thinning of the flame.
One of the main challenges in computational simulations of gas detonation propagation is that negative density or negative pressure may emerge during the time evolution, which will cause blow-ups.
The main and two bifurcated peaks exhibited negative propagation speeds relative to local flow velocity by consuming the remaining intermediates.
In particular, a critical Lewis number is found, below which negative propagation speeds do not exist while the 2D burning spots mentioned may be encountered.
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 front recedes from the axis of symmetry with a negative propagation speed that reaches a value as large as six times that of the freely propagating laminar flame with the same reactant concentrations found at the stoichiometric surface.
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