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Flame propagation is highlighted by an initial flame acceleration phase driven by turbulent burning in the cylinder wakes.
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Zn and Fe were determined by flame atomic absorption spectrometry (FAAS) in an air-acetylene flame using a UNICAM 939 Solaar atomic absorption spectrometer equipped with a deuterium background correction.
The results show that in these cases the initial envelope flame still remains envelope, but the evolution from an initial wake flame to an envelope flame is inhibited.
An initial envelope flame is found to remain envelope in time, and an initial wake flame is always transitioned into an envelope flame at a later time, with the normalized transition delay controlled by the initial Reynolds number and the initial Damkohler number.
This resulted in temporary extinction of the initial flame followed by re-ignition.
The initial flame shape is primarily determined by the initial Damkohler number, which has a critical value of Da0= 1.02.
However, they can be easily ignited by an open flame.
First, there is an initial stable regime, in which the flame is stabilized by thermo-diffusion and flame stretch, and the burning velocity is related to the Markstein length and rate of flame stretch.
In addition, it is found that the flame formation is initiated by autoignition with different ignition delays along the most reactive mixture fraction, instead of a flame propagation following an initial autoignition spot.
Radiative effects of the flame body are accounted for by a solid flame radiation model.
Turnover numbers of the hydroxylation of lauric acid at the ω and ω-1 positions by P450 4A11 were determined by a GC flame ionization detector (Shimadzu GC2010 instrument with a flame ionization detector).
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