Table 1:

Parameter values employed in simulations. The length of the long (top) leg of the flow loop L_Long = 1.98 mm. The driving pressure ΔP is chosen so that the transition from period-1 to higher orders of periodicity occurs at $T_{in}^{P+}$ = 1.04 sec, as in Fuerstman’s¹ experimental investigation.

	Bulk Fluid Viscosity μ (g cm−1 sec −1)	Surface Tension γ (dyn cm−1)	Fixed Tin Driving Pressure ΔP (dyn cm−2)	Fixed ΔP p1 Transition Time $T_{in}^{P+}$ (sec)	Radius R (μm)	Leg Length Ratio α LShort/LLong
Baseline	0.0295	3.6	32547	1.03	50	0.9
Low γ	0.0295	1.8	19400	0.525	50	0.9
High μ	0.059	3.6	38800	2.18	50	0.9
Low R	0.0295	3.6	73800	4.50	25	0.9
Low α	0.0295	3.6	18600	0.415	50	0.75
High α	0.0295	3.6	38600	1.25	50	0.98