<< Fire is not plasma becuase a condition for plasma is that ALL electrons are stripped from the atom. AFAIK, fire only has enough energy to strpi the outer shells most of the time. >>
Definition: A highly ionised gas in which the number of free electrons is approximately equal to the number of positive ions. Sometimes described as the fourth state of matter, plasmas occur in interstellar space, in the atmospheres of stars (including the sun), in discharge tubes, and in experimental thermonuclear reactors.
Because the particles of a plasma are charged, its behaviour differs in some respects from that of a gas. Plasmas can be created in the laboratory by heating a low-pressure gas until the mean kinetic energy of the gas particles is comparable to the ionisation potential of the gas atoms or molecules. At very high temperatures, from about 50 000 K upwards, collisions between gas particles cause cascading ionisation of the gas. However, in some cases, such as a fluorescent lamp, the temperature remains quite low as the plasma particles are continually colliding with the walls of the container, causing cooling and recombination. In such cases ionisation is only partial and requires a large energy input. In thermonuclear reactors, an enormous plasma temperature is maintained by confining the plasma away from the container walls using electromagnetic fields.
Thus, complete ionisation is not a requirement. In fact, only one electron needs to be removed from every atom for it to be a plasma, and there is enough energy for that.
<< Also, The colour from fire could be from 2 different things. First, certain metal ions have electron shell energy differences within the visible spectrum which means, if excited, it will emit a very pure spectral colour from the electron descending down a shell. Second, is due to temperature from balckbody radiation and this is emitted in a continuous spectrum depending on temperature. >>
Actually, if you look at the spectrum of a fire, you will see a blackbody distribution with the material absorption lines of whatever is in the gas.