The results of a number of laboratory tests of wind-driven fires indic
ate the existence of a characteristic wind speed, U'. The form of the
fire spread (V) as a function of mid-flame wind speed (U) differs abov
e and below this characteristic speed. The scatter in field data is so
great that it is difficult to confirm this result for field data. How
ever, expressions of the form: V/V(o) -1 = a(U/U')0.5 U/U' < 1 and V/V
(o) -1 = a(U/U')3 U/U' > 1 with U' = 2.5 m s-1 perform in a similar ma
nner to existing models. For many fuel types a = 15. A difficulty with
existing fire spread models is the measurement and definition of V(o)
, the no-wind rate of spread. It can hardly ever be measured in the fi
eld and has to be inferred from analytical formulae, or by extrapolati
ng measured data. The value of a depends on the method used estimate V
(o).