Figure 11:

Outlet periodicity for tube radii R = 50 μm (baseline case) and R = 25 μm for μ = 0.0295 g cm⁻¹ sec⁻¹, γ = 3.6 dyn cm⁻¹, and α = 0.9. In both cases the driving pressure is identical (ΔP = 32547 dyn cm⁻²), the increased fluidic resistance resulting by the decreased radius causes the transition from p₁ to higher orders to occur at a much larger T_in = 4.5 sec. Large symbols indicate transition region points.