Chaotic Streamlines Inside Droplet Radoslav Bozinoski
System • Neutrally Buoyant – External Flow • Vorticity • Rate of Strain Tensor • Linear – Internal Flow • Nonlinear • Chaotic Streamlines
Flow field • Coordinate system moving with center-of- mass. • Inter-boundary tension is sufficiently large to maintain a spherical drop shape. • Far from the drop the fluid is assumed to undergo a steady linear motion
Governing Equations ∞ x = U 1 2 w × x E ⋅ x u u x = 1 2 − 3 E ⋅ x − 2 x x ⋅ E ⋅ x ] 1 2 [ 5r 2 w × x E = − 1 1 / 1 a 0 0 E 22 a = 0 a / 1 a 0 E 11 0 0
Simplifications x y , y x ,a 1 a 0 ≤ a ≤ 1 w = w x ,w y ,w z − w y , − w x , − w z x − x ,w y − w y ,w z − w z w z ≥ 0 z − z , w x − w x , w y − w y w y ≥ 0
Parameters of interest • a = 1 - Axisymmetric • ω = (ωx,0,ωz) – ω = 0 – ω - inline with z-axis – ω - oriented off z-axis
ω = 0 a = 1.0 w = (0,0,0 ) LCE = (0,0,-) Dot - Saddle fixed points Asterisks – Elliptic fixed points ψ = 0 -Nested family of tori
ω - inline with z-axis • ψ exists t = t 0
ω – oriented off z-axis • Chaotic Streamlines –Fixed orientation (36º) –Fixed ω magnitude • a = 1.0 • ω = 0.1 • ω = ( wx,0,wz) • ω = 2.0
Theta = 36º
ω = 0.1
ω = 2.0
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