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The maximum burning rate enhancement factor, defined as the ratio of the parameter for interacting fires to non-interacting ones, was shown to be 2.3.
For unity Lewis number, it is shown that the maximum burning rate measured in a one-dimensional planar stoichiometric premixed flame may be used as a reference for a diffusion flame close to extinction and also later when edge flames and triple flames are formed.
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For cases with the same wind velocity, the burning rate reaches the maximum value at a small spacing distance (rather than the case with attached pools), where air entrainment restriction is relatively weaker and the radiation feedback is at a higher level.
And the maximum detection distance grows with the growth of burning rate.
Then, the other data related to the propellants to be measured for the burning rate, such as energy level of the propellant, the propellant density, the maximum combustion temperature, and the physical sizes of the propellants, were inputted to the computer of the burning rate measurement device.
It has been found that the burning rate varies along the radial direction and the mass and heat transfer around the pool peripheral is maximum and most influential.
Addition of nitrocellulose (NC) particles to the nanofuel diminishes or fully counteracts the burning rate decreases and provides a means of tuning the burning rate constant higher than that of pure Kerosene (maximum 13.8% increase over control with 2.3 wt% nAl and 0.6 wt% NC added).
The pressure propels the projectile and increases the burning rate.
Same storage size, but faster burning rate.
Downstream, the burning rate gradually increases.
Thus, the burning rate was increased.
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