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An ultimate quenching extinction limit is found at low stretch with sufficiently high induced heat losses.
This flame is quenched either by radiation heat loss at low stretch rate or by incomplete combustion with an excessive stretch.
In addition, gas radiation can cause a substantial decrease of flame temperature and constitutes a significant portion of the heat feedback to the solid at low stretch rates.
The extinction behavior at low stretch rates is qualitatively similar to that predicted by earlier theory with only surface radiation loss.
Numerical calculation including radiative heat loss from the flame zone qualitatively agreed with the experimental results and indicated that the mechanism of counterflow diffusion flame extinction at low stretch rates was radiative heat loss.
In addition, flame bifurcation at low stretch rates and at ϕ = 0.58 and 0.60 were experimentally observed for the present low-Lewis-number mixture, indicating the validity of the previous computational and theoretical studies on the G-shaped extinction curve of planar counterflow flames.
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(i) At low stretching ratio, in the linear deformation regime, reinforcement is driven by the primary network filler structure.
It is shown here for the first time that 1-D models are remarkably accurate at low stretching speeds but fail at high stretching speeds.
At low stretching temperatures and high rates the stress optical behavior was found to start with an initial glassy photo elastic behavior.
The slight deviations at low stretching forces are due to protein−protein and protein−DNA aggregation (24).
Drawing at a high temperature shows rapid crystalline orientation development, even at a low stretch ratio of 1.5, while molecular alignment develops steadily in the amorphous phase.
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