Now we need to consider another point. Flame or fire is entirely 'quenched' in a vacuum. This is significant. If these flames are simply a collection of magnetic dipoles that have lost their 'orderliness' so to speak - in the field, then if they are placed in a vacuum or in some sort of chamber where 'ignitable' compounds or gases are omitted - then the flame literally 'burns out' and the fire is prevented.
To me this suggests that the binding fields of these magnetic dipoles only unravel to the extent that there is another medium to which they can progress. And as atoms and particles are the 'things' that are absent in a vacuum - I can safely conclude that they need to move towards atoms and molecules. Whatever the resulting 'amalgam' or dissassociated state of the particles in the 'flame' they will only move towards some 'housing' some area that - at it's least - has other atoms and molecules. And, in as much as fire is known to exaserbate the carbon dioxide content of our atmosphere then this, also at its least may be the 'housing' required by some of these particles from the 'flame'. In other words they move away from their first field and reconjoin in new fields creating new molecules of carbon dioxide, for example, again extraneous to the atoms - but allowing a balanced distribution of charge that somehow satisfies the valence condition of two or more otherwise disassociated atoms.
To me this suggests that the binding fields of these magnetic dipoles only unravel to the extent that there is another medium to which they can progress. And as atoms and particles are the 'things' that are absent in a vacuum - I can safely conclude that they need to move towards atoms and molecules. Whatever the resulting 'amalgam' or dissassociated state of the particles in the 'flame' they will only move towards some 'housing' some area that - at it's least - has other atoms and molecules. And, in as much as fire is known to exaserbate the carbon dioxide content of our atmosphere then this, also at its least may be the 'housing' required by some of these particles from the 'flame'. In other words they move away from their first field and reconjoin in new fields creating new molecules of carbon dioxide, for example, again extraneous to the atoms - but allowing a balanced distribution of charge that somehow satisfies the valence condition of two or more otherwise disassociated atoms.
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