Deep sea divers suffer from decompression sickness (DCS) when their rate of
ascent to the surface is too rapid. When the ambient pressure drops, inert
gas bubbles may form in blood vessels and tissues. The evolution of a gas
bubble in a rigid tube filled with slowly moving fluid, intended to simulat
e a bubble in a blood vessel, is studied by solving a coupled system of flu
id-flow and gas transport equations. The governing equations for the fluid
motion are solved using two techniques: an analytical method appropriate fo
r small nondeformable spherical bubbles, and the boundary element method fo
r deformable bubbles of arbitrary size, given an applied steady flow rate.
A steady convection-diffusion equation is then solved numerically to determ
ine the concentration of gas. The bubble volume, or equivalently the gas ma
ss inside the bubble for a constant bubble pressure, is adjusted over time
according to the mass flux at the bubble surface. Using a quasi-steady appr
oximation, the evolution of a gas bubble in a tube is obtained. Results sho
w that convection increases the gas pressure gradient at the bubble surface
, hence increasing the rate of bubble evolution. Comparing with the result
for a single gas bubble in an infinite tissue, the rare of evolution in a t
ube is approximately twice as fast. Surface tension is also shown to have a
significant effect. These findings may have important implications for our
understanding of the mechanisms of inert gas bubbles in the circulation un
derlying decompression sickness.