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Fig. 15
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Evolution of dimensionless parameters for a thermal propagat ing in a turbulent environment (cf. Turner 1962). 
, 
, 
, w1 =w/u0, and f = b3g′/F*, with F*, = b3g′0 The simulation truncates when b1 → 0, indicating that its entire initia buoyancy perturbation has detrained into the environment.
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