Abstract
The linear-temporal and spatiotemporal instability behavior of a confined gas–liquid shear flow was investigated theoretically. The practical situation which motivated this investigation is the recessed gas–liquid shear coaxial injector, usually used in liquid propellant rocket engines. The corresponding dispersion relation between the complex wave growth rate and the complex wave number was derived. The temporal stability analysis shows that a more strongly confined gas–liquid shear flow exhibits a larger temporal growth rate than a weakly confined gas– liquid shear flow. A larger nondimensional outer injector radius, a larger liquid-to-gas density ratio and velocity ratio, and a smaller liquid Weber number would stabilize the confined gas–liquid shear flow. In spatiotemporal mode,whentheconfinementisstrong, flowisabsolutelyunstable.Whentheconfinementbecomesweak,the flowcan transit to become convectively unstable. Under strong confinement, the confined jet is always absolutely unstable independent of the variation of liquid–gas density ratio, velocity ratio, and liquid Weber number, i.e., the confinement is the most key parameter determining the absolutely/convectively unstable characteristics of the flow. However, the absolute growth rate and wavelength can be affected by these parameters.
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