A soap film has two air-water interfaces. The Young–Laplace equation therefore gives
The radius is half the specified diameter; using the single-interface droplet expression would miss a factor of two.
For the same ideal gas composition and temperature, , hence . The bubble volume is . The gas's mass in excess of displaced ambient air is
This is a positive buoyant mass, meaning a net downward weight after subtracting ordinary air buoyancy. It is not an upward lifting capacity. Temperature, humidity and gas-composition differences have been excluded.
Treat the two film surfaces as an effective interfacial tension . The relevant Bond number for the gas-density difference is . Substituting the Young–Laplace equation and the preceding density relation gives
Thus the formal crossover gives . This compares gravity on the excess gas with capillary restoration and neglects film weight. It does not say gravity-driven drainage of a real water film is negligible below kilometre scales. At this enormous radius, treating ambient pressure and density as uniform is itself no longer quantitatively reliable.
Approximating the skin as a uniform thin water shell with density ,
This is about 2500 times the buoyant mass of the enclosed gas. The film weight therefore dominates the bubble's downward gravitational force under the stated assumptions. Equal-temperature air inside does not provide a net lift to balance it: an apparently floating bubble can be transiently supported by air currents or have different internal temperature/composition. Film thickness is generally nonuniform and changes with drainage and evaporation; the uniform thickness is an estimate, not a stable equilibrium condition.

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