The size and number of bubbles produced by the desorption of supersatu
rated gases from water are shown to be a primary function of the energ
y available for bubble formation in a flowing system; this energy is t
hat not dissipated in turbulence and friction. The number of nucleatio
n sites is greatly increased when certain impurities are present, part
icularly surface-active agents. Low saturation pressures can produce v
ery large numbers of very small bubbles when added energy is provided
for discharge. High gas concentrations produce excess large bubbles wh
ich pass up rapidly through the much slower rising bubble mass. A comb
ination of low saturation pressure followed by higher pressure for flo
w, such as by liquid pumping, results in bubble characteristics which
can be controlled for applications.