[S0022-1481(00)03102-9]

Table 3, which follows, was inadvertently omitted from the originally published paper.

Table
Summary of self-preserving properties of plane buoyant turbulent plumesa
SourcePlume TypeZ/bxxo/bZ/lfminxxo/lMlf/xxoFmaxf¯max/f¯max
PresentAdiabatic Wall9392–1557.912–210.0765.710.37
Lai et al. (1986)bAdiabatic Wall3810–38 10.8 1–5 0.0936.800.34
Grella and Faeth (1973)b,cAdiabatic Wall13.00.0777.50
Liburdy and Faeth (1978) and Liburdy et al. (1979)b,cIsothermal Wall5.90.1125.200.25
Sangras et al. (1998)Free Line9376–1552.6d 9–210.1202.100.47
aPlane buoyant turbulent plumes in still and unstratified environments. Wall plumes are along vertical smooth surfaces. Range of streamwise distances are for conditions where measurements were made over the cross section of the plumes. Adiabatic wall plume entries are ordered chronologically.
bThese flows were evolving over the range of the measurements so that the values of lf/xxo,Fmax, and f¯max/f¯max pertain to results obtained farthest from the source.
cSource was a linear array of round jets so that slot properties cannot be defined.
dThis value is Z/2lfmin, which is the full characteristic width of the flow, similar to the other entries in this column.
Summary of self-preserving properties of plane buoyant turbulent plumesa
SourcePlume TypeZ/bxxo/bZ/lfminxxo/lMlf/xxoFmaxf¯max/f¯max
PresentAdiabatic Wall9392–1557.912–210.0765.710.37
Lai et al. (1986)bAdiabatic Wall3810–38 10.8 1–5 0.0936.800.34
Grella and Faeth (1973)b,cAdiabatic Wall13.00.0777.50
Liburdy and Faeth (1978) and Liburdy et al. (1979)b,cIsothermal Wall5.90.1125.200.25
Sangras et al. (1998)Free Line9376–1552.6d 9–210.1202.100.47
aPlane buoyant turbulent plumes in still and unstratified environments. Wall plumes are along vertical smooth surfaces. Range of streamwise distances are for conditions where measurements were made over the cross section of the plumes. Adiabatic wall plume entries are ordered chronologically.
bThese flows were evolving over the range of the measurements so that the values of lf/xxo,Fmax, and f¯max/f¯max pertain to results obtained farthest from the source.
cSource was a linear array of round jets so that slot properties cannot be defined.
dThis value is Z/2lfmin, which is the full characteristic width of the flow, similar to the other entries in this column.